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  2. preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/README.md +18 -0
  3. preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/application.tex +204 -0
  4. preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/correction.tex +295 -0
  5. preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/cyclic-obstruction.tex +406 -0
  6. preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/division-realization.tex +240 -0
  7. preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/formal-generic.tex +406 -0
  8. preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/generation.tex +310 -0
  9. preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/global-defect.tex +298 -0
  10. preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/introduction.tex +139 -0
  11. preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/lifting.tex +81 -0
  12. preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/linkage.tex +317 -0
  13. preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/responses.tex +312 -0
  14. preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/transfer.tex +250 -0
  15. preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/paper.pdf +3 -0
  16. preprints/A-Counterexample-to-Rysers-Covering-Conjecture-September-23-2026/README.md +18 -0
  17. preprints/A-Counterexample-to-Rysers-Covering-Conjecture-September-23-2026/build/construction.tex +857 -0
  18. preprints/A-Counterexample-to-Rysers-Covering-Conjecture-September-23-2026/build/figures/two-coordinates.tex +19 -0
  19. preprints/A-Counterexample-to-Rysers-Covering-Conjecture-September-23-2026/build/incidence.tex +707 -0
  20. preprints/A-Counterexample-to-Rysers-Covering-Conjecture-September-23-2026/build/linecover.tex +447 -0
  21. preprints/A-Counterexample-to-Rysers-Covering-Conjecture-September-23-2026/build/paper.tex +301 -0
  22. preprints/A-Counterexample-to-Rysers-Covering-Conjecture-September-23-2026/build/references.bib +390 -0
  23. preprints/A-Counterexample-to-Rysers-Covering-Conjecture-September-23-2026/build/selection.tex +538 -0
  24. preprints/A-Counterexample-to-Rysers-Covering-Conjecture-September-23-2026/paper.pdf +3 -0
  25. preprints/A-Counterexample-to-Walls-D2-Problem-October-6-2026/README.md +18 -0
  26. preprints/A-Counterexample-to-Walls-D2-Problem-October-6-2026/build/figures/tower.tex +20 -0
  27. preprints/A-Counterexample-to-Walls-D2-Problem-October-6-2026/build/main.tex +20 -0
  28. preprints/A-Counterexample-to-Walls-D2-Problem-October-6-2026/build/preamble.tex +27 -0
  29. preprints/A-Counterexample-to-Walls-D2-Problem-October-6-2026/build/references.bib +148 -0
  30. preprints/A-Counterexample-to-Walls-D2-Problem-October-6-2026/build/sections/01-introduction.tex +131 -0
  31. preprints/A-Counterexample-to-Walls-D2-Problem-October-6-2026/build/sections/02-tower.tex +257 -0
  32. preprints/A-Counterexample-to-Walls-D2-Problem-October-6-2026/build/sections/03-plus.tex +117 -0
  33. preprints/A-Counterexample-to-Walls-D2-Problem-October-6-2026/build/sections/04-construction.tex +189 -0
  34. preprints/A-Counterexample-to-Walls-D2-Problem-October-6-2026/wall-d2-counterexample.pdf +3 -0
  35. preprints/A-Counterexample-to-the-Group-Ring-Determinant-Conjecture-September-23-2026/README.md +18 -0
  36. preprints/A-Counterexample-to-the-Group-Ring-Determinant-Conjecture-September-23-2026/build/main.tex +615 -0
  37. preprints/A-Counterexample-to-the-Group-Ring-Determinant-Conjecture-September-23-2026/build/references.bib +108 -0
  38. preprints/A-Counterexample-to-the-Group-Ring-Determinant-Conjecture-September-23-2026/paper.pdf +3 -0
  39. preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/README.md +20 -0
  40. preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/build/figures/double-ray.tex +30 -0
  41. preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/build/paper.tex +99 -0
  42. preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/build/references.bib +83 -0
  43. preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/build/sections/01-introduction.tex +202 -0
  44. preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/build/sections/02-matroids.tex +119 -0
  45. preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/build/sections/03-filters.tex +278 -0
  46. preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/build/sections/04-local-bases.tex +332 -0
  47. preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/build/sections/05-assembly.tex +342 -0
  48. preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/build/sections/06-counterexample.tex +153 -0
  49. preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/build/sections/07-consequences.tex +48 -0
  50. preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/paper.pdf +3 -0
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+ preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/A-counterexample-to-Naimarks-problem-in-ZFC-September-24-2026/naimark-counterexample-zfc.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/A-Counterexample-to-Rysers-Covering-Conjecture-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/A-counterexample-to-Sidorenkos-conjecture-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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+ preprints/A-counterexample-to-Tachikawas-second-conjecture-September-23-2026/paper.pdf filter=lfs diff=lfs merge=lfs -text
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preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/README.md ADDED
@@ -0,0 +1,18 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
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+ # [A Counterexample to Kurosh’s Division-Ring Problem](paper.pdf)
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+
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+ **Author:** OpenAI
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+
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+ **Date:** September 23, 2026
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+
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+ ## Citation
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+
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+ ```bibtex
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+ @misc{OAI:A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026,
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+ author = {{OpenAI}},
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+ title = {{A Counterexample to Kurosh's Division-Ring Problem}},
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+ howpublished = {OpenAI Math Release preprint
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+ \href{https://github.com/openai/math/blob/main/preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/paper.pdf}{OAI:A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026}},
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+ year = {2026}
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+ }
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+ ```
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+
preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/application.tex ADDED
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+ \section{The countable construction and the actual center}
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+ \label{sec:countable-construction}
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+
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+ We now apply Theorem~\ref{thm:lifting} repeatedly. Recall its
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+ full conclusion: from a finite-dimensional central division algebra $A/k$
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+ and a tuple of free series $X$ whose constant term generates $A$ and whose
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+ two linear coefficients are independent modulo inner directions, it
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+ produces such a tuple over a countable extension $k'$ and a central
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+ division algebra of strictly larger degree. It preserves every old
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+ polynomial identity and gives a monic algebraic relation for any chosen
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+ series $w$. The countability, generation, and two-direction conclusions
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+ are all needed to iterate this theorem.
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+
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+ The resulting division algebras need not embed in one another. We use
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+ an ultraproduct to retain their polynomial relations, and then prove
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+ separately that the resulting algebra has infinite dimension over its
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+ actual center.
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+
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+ \subsection{Scheduling all polynomial expressions}
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+
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+ Start with
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+ \[
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+ k_0=\overline{\mathbb Q},\qquad A_0=k_0,\qquad
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+ X^{(0)}=(z_1,z_2).
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+ \]
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+ Its constant pair $(0,0)$ generates $k_0$ as a unital $k_0$-algebra.
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+ The inner-direction space is zero, and its two linear coefficients
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+ $(1,0)$ and $(0,1)$ are independent. Thus it satisfies the hypotheses
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+ of Theorem~\ref{thm:lifting}.
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+
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+ Inductively we obtain countable fields
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+ \[
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+ k_0\subseteq k_1\subseteq k_2\subseteq\cdots,
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+ \]
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+ finite-dimensional central division algebras $A_i/k_i$ of strictly
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+ increasing degrees, and pairs
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+ \[
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+ X^{(i)}\in A_i\langle\!\langle z_1,z_2\rangle\!\rangle^2
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+ \]
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+ satisfying the same generation and transverse-independence hypotheses.
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+ Write $(x_i,y_i)=X^{(i)}_0$ for the constant pair; in particular,
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+ \begin{equation}
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+ A_i=k_i[x_i,y_i].
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+ \label{eq:stage-generation}
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+ \end{equation}
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+
47
+ Here is a schedule that ensures algebraicity of every expression
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+ needed in the limit. When $k_i$ has been constructed, enumerate the
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+ countable set $k_i\langle x,y\rangle$ as
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+ $(p_{i,j})_{j\geq0}$. Enumerate the pairs $(i,j)\in\mathbb N^2$ by
51
+ increasing $i+j$, in a fixed order within each diagonal. If $(i_n,j_n)$
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+ is the $n$th pair, beginning at $n=0$, then $i_n\leq n$.
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+ At stage $n$, apply the lifting theorem to
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+ \[
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+ w=p_{i_n,j_n}(X^{(n)}).
56
+ \]
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+ This expression is defined over $k_n$, since $k_{i_n}\subseteq k_n$.
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+ The identity $w-p_{i_n,j_n}(X^{(n)})=0$ is preserved, so the new relation
59
+ for the lifted $w$ gives a nonzero monic polynomial
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+ \[
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+ q_{i_n,j_n}(t)\in k_{n+1}[t]
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+ \]
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+ such that
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+ \begin{equation}
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+ q_{i_n,j_n}\bigl(p_{i_n,j_n}(X^{(n+1)})\bigr)=0.
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+ \label{eq:retained-formal-relation}
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+ \end{equation}
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+ Every later lifting preserves this polynomial identity, now regarded
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+ over its coefficient field $k_{n+1}$. Taking constant terms shows that
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+ the corresponding identity holds at $(x_h,y_h)$ for every $h\geq n+1$.
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+ Each polynomial over each $k_i$ is treated at a finite stage.
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+
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+ \subsection{A two-generated algebraic division ring}
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+
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+ Fix a nonprincipal ultrafilter $\mathcal U$ on $\mathbb N$ and form
76
+ (see \cite{Keisler2010} for the general construction)
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+ \[
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+ \mathcal D=\prod_{i\geq0} A_i\big/\mathcal U.
79
+ \]
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+ Here two sequences represent the same element when their equality set
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+ belongs to $\mathcal U$. This is a division ring: a nonzero class has
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+ nonzero coordinates on a set in $\mathcal U$, and taking their
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+ coordinatewise inverses on that set gives its inverse.
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+
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+ Put $k_\infty=\bigcup_i k_i$. An element $c\in k_j$ determines a class
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+ in $\mathcal D$ by taking its image in the central field $k_i\subset A_i$
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+ for $i\geq j$ and choosing arbitrary coordinates at the finitely many
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+ earlier indices. These classes are independent of the early choices
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+ and of $j$. They define a central field embedding
90
+ \[
91
+ k_\infty\hookrightarrow\mathcal D:
92
+ \]
93
+ the field operations agree at every sufficiently large index, and a
94
+ nonzero field element stays nonzero at all those indices. This
95
+ construction uses only the inclusions of coefficient fields; it does
96
+ not require embeddings between the algebras $A_i$.
97
+
98
+ Let
99
+ \[
100
+ x=[(x_i)_i],\qquad y=[(y_i)_i],\qquad
101
+ R=k_\infty[x,y]\subseteq\mathcal D.
102
+ \]
103
+ Every $r\in R$ has the form $p(x,y)$ for some
104
+ $p\in k_j\langle x,y\rangle$. The schedule and
105
+ \eqref{eq:retained-formal-relation} provide a nonzero monic polynomial
106
+ $q\in k_h[t]$, for a suitable $h$, such that
107
+ $q(p(x_i,y_i))=0$ at every sufficiently large index. Therefore
108
+ $q(r)=0$ in $\mathcal D$. Every element of $R$ is algebraic over
109
+ $k_\infty$.
110
+
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+ This already makes $R$ a division ring. For $0\ne r\in R$, choose a
112
+ nonzero relation of least degree
113
+ \[
114
+ a_0+a_1r+\cdots+a_nr^n=0,
115
+ \qquad a_j\in k_\infty.
116
+ \]
117
+ Its constant coefficient is nonzero: otherwise multiplication by
118
+ $r^{-1}$ in the ambient division ring $\mathcal D$ would give a shorter
119
+ relation. Consequently
120
+ \[
121
+ r^{-1}=-a_0^{-1}(a_1+a_2r+\cdots+a_nr^{n-1})\in R.
122
+ \]
123
+ Since $k_\infty$ is countable and $R$ is generated by two elements as an
124
+ algebra, $R$ is countable. Its characteristic is zero.
125
+
126
+ \subsection{Infinite dimension and passage to the center}
127
+
128
+ We first prove
129
+ \begin{equation}
130
+ [R:k_\infty]=\infty.
131
+ \label{eq:infinite-auxiliary-dimension}
132
+ \end{equation}
133
+ For each $i$ and $\ell\geq0$, let $V_{i,\ell}$ be the $k_i$-span of the
134
+ words in $x_i,y_i$ of length at most $\ell$, including the empty word
135
+ $1$. If $V_{i,\ell}=V_{i,\ell+1}$, then $V_{i,\ell}$ is stable under
136
+ right multiplication by $x_i$ and $y_i$ and contains every word.
137
+ By \eqref{eq:stage-generation}, it equals $A_i$. Until this happens,
138
+ the dimensions increase strictly, starting from $1$.
139
+
140
+ Fix $\ell$. The dimensions $[A_i:k_i]$ tend to infinity, so
141
+ \[
142
+ \dim_{k_i}V_{i,\ell}\geq\ell+1
143
+ \]
144
+ for every sufficiently large $i$. There are only finitely many
145
+ subsets of size $\ell+1$ in the finite list of words of length at most
146
+ $\ell$. The ultrafilter therefore selects one fixed subset
147
+ $w_0,\ldots,w_\ell$ that is linearly independent at a set of stages
148
+ belonging to $\mathcal U$.
149
+
150
+ These same words are independent over the embedded $k_\infty$ in $R$.
151
+ Indeed, the coefficients of a putative relation
152
+ \[
153
+ \sum_{j=0}^{\ell} c_j w_j(x,y)=0
154
+ \]
155
+ all belong to one field $k_h$. Equality in the ultraproduct holds on
156
+ a set in $\mathcal U$. Intersecting it with the independence set and
157
+ the tail $i\geq h$ gives a nonempty set where stage independence
158
+ forces every $c_j$ to vanish. Thus $R$ has arbitrarily large finite
159
+ linearly independent sets, proving
160
+ \eqref{eq:infinite-auxiliary-dimension}.
161
+
162
+ Finally let $F=Z(R)$ be the actual center. It contains $k_\infty$ and
163
+ is algebraic over $k_\infty$, since every element of $R$ is. In
164
+ particular, every element of $R$ is algebraic over $F$. Also
165
+ \[
166
+ R=k_\infty[x,y]=F[x,y]=F(x,y),
167
+ \]
168
+ because $F\subseteq R$ and $R$ is already a division ring.
169
+
170
+ We use finite descent of the multiplication table and generator
171
+ coordinates; compare the proof of the local-finiteness criterion in
172
+ \cite[Section~4]{DeoBienHai2019}. Suppose, for a contradiction, that
173
+ $[R:F]=n<\infty$. Choose an
174
+ $F$-basis $b_1=1,b_2,\ldots,b_n$ of $R$, and write
175
+ \[
176
+ b_i b_j=\sum_{h=1}^n c_{ijh}b_h,
177
+ \qquad
178
+ x=\sum_{h=1}^n u_hb_h,
179
+ \qquad
180
+ y=\sum_{h=1}^n v_hb_h,
181
+ \]
182
+ with all coefficients in $F$. Let $E$ be the subfield of $F$
183
+ generated over $k_\infty$ by these finitely many coefficients.
184
+ Algebraicity gives $[E:k_\infty]<\infty$. The space
185
+ \[
186
+ B=\sum_{h=1}^n E b_h
187
+ \]
188
+ contains $1,x,y$ and is closed under multiplication by the displayed
189
+ structure constants. It is therefore a $k_\infty$-subalgebra of $R$
190
+ containing $k_\infty[x,y]=R$, so $B=R$. This implies
191
+ \[
192
+ [R:k_\infty]\leq n[E:k_\infty]<\infty,
193
+ \]
194
+ contrary to \eqref{eq:infinite-auxiliary-dimension}.
195
+
196
+ Thus the countable characteristic-zero division ring $D=R$ is
197
+ algebraic over its actual center $F$, while
198
+ \[
199
+ D=F[x,y]=F(x,y),\qquad [D:F]=\infty.
200
+ \]
201
+ The finite set $\{x,y\}$ witnesses the failure of local finiteness.
202
+
203
+ This proves Theorem~\ref{thm:main}, subject only to Theorem~\ref{thm:lifting},
204
+ which we now prove.
preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/correction.tex ADDED
@@ -0,0 +1,295 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Solving the free-series equations}
2
+ \label{sec:free-correction}
3
+
4
+ We now use the response and cyclic-sum results to keep the output of a
5
+ substitution conjugate to its constant term. The input retains two prescribed
6
+ linear coefficients. This is the point at which free words, rather than
7
+ commuting parameters, enter the construction essentially.
8
+
9
+ Work over a common split scalar field $E$ in which the preceding evaluations
10
+ and spectral projections are defined. All series substitutions below have
11
+ small constant terms and are interpreted by the coefficientwise valuation
12
+ convergence established earlier. In particular, the letters of a free series
13
+ commute with its matrix coefficients; the letters do not commute with each
14
+ other.
15
+
16
+ Put $m=11$ and index the blocks by $i\in\mathbb Z/m\mathbb Z$.
17
+ Let $P_i$ be jointly independent small generic pairs of $b\times b$
18
+ matrices. Set $R=\operatorname{diag}(P_i)$, a pair of $mb\times mb$
19
+ matrices. The old coefficient algebra acts on a separate factor of dimension
20
+ $d$. Write $\lambda_{i,h}$ and $\pi_{i,h}$ for the distinct eigenvalues
21
+ and spectral projections of $w(P_i)$. Eigenvalues belonging to different
22
+ blocks are distinct. For a substitution $Z$ with constant term $R$, let
23
+ $S_{i,h}(Z)$ denote the fixed-root Schur expression at $\lambda_{i,h}$,
24
+ using the constant projection $\pi_{i,h}$ in the $i$-th block.
25
+
26
+ We recall precisely the response information needed here. In each block
27
+ choose one eigenvalue label from every part of the active partition, giving
28
+ $a$ selected labels. The selected loop-response map is
29
+ \[
30
+ D_i:M_b(E)^2\longrightarrow E^a.
31
+ \]
32
+ Put $L_i=\operatorname{im}D_i$ and $H_i=E^a/L_i$.
33
+ Proposition~\ref{prop:compatible-relations} supplies a vector space
34
+ $G=\mathcal G$ of dimension $g$ and coordinate isomorphisms
35
+ \[
36
+ p_i:G\longrightarrow H_i^*.
37
+ \]
38
+ For a generic fixed input arrow $U$ on $i\leftarrow j$, varying its
39
+ opposite arrow $V$ gives two selected responses
40
+ \[
41
+ m_i(U,V)\in E^a,
42
+ \qquad m_j(V,U)\in E^a.
43
+ \]
44
+ The annihilator of these paired responses in $H_i^*\oplus H_j^*$ is
45
+ exactly
46
+ \begin{equation}
47
+ \{(p_i(c),p_j(c)):c\in G\}.
48
+ \label{eq:correction-paired-annihilator}
49
+ \end{equation}
50
+ The identifications $p_i$ are compatible for the whole collection of blocks
51
+ and for all the generic arrows used below.
52
+
53
+ The transfer result supplies the following additional facts. If all Schur
54
+ expressions vanish in degrees less than $\ell$, their degree-$\ell$
55
+ coefficients are scalar on the projected eigenspaces. The resulting tuples
56
+ belong to their active spaces and are determined by their selected entries.
57
+ Denote the selected error for a word $\omega$ of length $\ell$ in block
58
+ $i$ by $e_{i,\omega}\in E^a$. The cyclic-sum result says that, for every
59
+ orbit $\mathcal O$ of words under cyclic rotation,
60
+ \begin{equation}
61
+ \sum_{\omega\in\mathcal O}\sum_i
62
+ p_i(c)\bigl(e_{i,\omega}+L_i\bigr)=0
63
+ \qquad(c\in G).
64
+ \label{eq:correction-cyclic-input}
65
+ \end{equation}
66
+ These statements hold for every partial substitution under consideration,
67
+ including after an extension of its scalar field. The preceding results
68
+ therefore supply all the hypotheses used in the next construction.
69
+
70
+ \begin{proposition}
71
+ \label{prop:eleven-block-correction}
72
+ Prescribe generic input-arrow pairs on the edges
73
+ \[
74
+ \begin{array}{c|c}
75
+ \text{letter}&\text{offsets }i-j\text{ of edges }i\leftarrow j\\ \hline
76
+ s_1&1,2\\
77
+ s_2&3,4.
78
+ \end{array}
79
+ \]
80
+ Under the response and cyclic-sum hypotheses above, there is a pair
81
+ $Z(s_1,s_2)\in M_{mb}(E)\langle\!\langle s_1,s_2\rangle\!\rangle^2$
82
+ with constant term $R$ and exactly these prescribed linear coefficients,
83
+ for which
84
+ \[
85
+ S_{i,h}(Z)=0\qquad\text{for every }i,h.
86
+ \]
87
+ It can be constructed by finite linear systems. At step $\ell\ge3$ the
88
+ new unknowns are coefficients of degree $\ell-1$ on the reverse edges
89
+ and coefficients of degree $\ell$ on the diagonal blocks.
90
+ \end{proposition}
91
+
92
+ \begin{proof}
93
+ None of the four forward offsets is zero. The sum of two forward offsets
94
+ lies between $2$ and $8$, and is therefore nonzero modulo $11$.
95
+ Thus a path of one or two forward steps cannot return to its initial block.
96
+ Constant input steps preserve each block. The path expansions for the
97
+ output and for its Schur expressions consequently show that the prescribed
98
+ constant and linear terms, with zero higher coefficients, solve all the
99
+ Schur equations through degree two.
100
+
101
+ Suppose a partial substitution solves them in degrees less than
102
+ $\ell\ge3$. Add a correction $V B$ on a reverse edge $j\leftarrow i$,
103
+ where $B$ is a word of length $\ell-1$, and add arbitrary degree-$\ell$
104
+ loop corrections. At the block-diagonal constant term, an off-diagonal
105
+ input variation gives an output variation in the same off-diagonal block.
106
+ Its compression on any fixed root block is zero. Thus the reverse
107
+ correction changes no Schur equation through degree $\ell-1$.
108
+
109
+ Its contribution in degree $\ell$ must pair it with a single prescribed
110
+ linear arrow. There is a unique forward edge that returns along this
111
+ reverse edge: the reverse offsets $10,9,8,7$ correspond respectively to
112
+ $1,2,3,4$. If that edge has coefficient $U$ and color $s_c$, the
113
+ contributions are
114
+ \begin{equation}
115
+ \begin{array}{c|c|c}
116
+ \text{block}&\text{word}&\text{selected response}\\ \hline
117
+ i&s_cB&m_i(U,V)\\
118
+ j&Bs_c&m_j(V,U).
119
+ \end{array}
120
+ \label{eq:correction-leading-pair}
121
+ \end{equation}
122
+ This is exactly the two-arrow Schur calculation defining the paired
123
+ responses. A previously present coefficient of degree at least two
124
+ cannot interact with the new degree-$\ell-1$ coefficient in degree
125
+ $\ell$. Two new corrections have total degree at least
126
+ $2(\ell-1)>\ell$. The degree-$\ell$ variation is therefore linear.
127
+ Loop corrections give $D_i$ independently at every vertex and every
128
+ word of length $\ell$.
129
+
130
+ We compute the annihilator of this finite correction map. Let
131
+ $f_{i,\omega}\in(E^a)^*$ be a collection of functionals annihilating its
132
+ image. The loop columns first imply that $f_{i,\omega}$ annihilates
133
+ $L_i$. Write its induced functional on $H_i$ uniquely as
134
+ \[
135
+ f_{i,\omega}=p_i(c_{i,\omega}),\qquad c_{i,\omega}\in G.
136
+ \]
137
+ Here and below we use the same notation for the induced functional and
138
+ its pullback to $E^a$. By
139
+ \eqref{eq:correction-paired-annihilator} and
140
+ \eqref{eq:correction-leading-pair}, annihilation of the reverse columns
141
+ is equivalent to
142
+ \begin{equation}
143
+ c_{i,s_cB}=c_{j,Bs_c}
144
+ \quad\text{on every edge }i\leftarrow j\text{ of color }c.
145
+ \label{eq:correction-edge-equality}
146
+ \end{equation}
147
+ The two offsets of either color are consecutive integers, say $a,a+1$.
148
+ Applying \eqref{eq:correction-edge-equality} to both edges out of $j$
149
+ gives
150
+ \[
151
+ c_{j+a,s_cB}=c_{j+a+1,s_cB}.
152
+ \]
153
+ As $j$ ranges over $\mathbb Z/11\mathbb Z$, this makes the value
154
+ independent of the vertex. Equation~\eqref{eq:correction-edge-equality}
155
+ then identifies its value with that on the rotated word $Bs_c$.
156
+ Iterating rotations shows that the annihilator consists exactly of one
157
+ element of $G$ per cyclic orbit of words. The converse follows from
158
+ the same paired-annihilator identity.
159
+
160
+ Equation~\eqref{eq:correction-cyclic-input} says that every such
161
+ annihilator kills the degree-$\ell$ error. Finite-dimensional linear
162
+ duality therefore puts the negative error in the image of the correction
163
+ map. Choose a correction solving all selected equations. Lower degrees
164
+ remain solved, so transfer and the active partition imply that every
165
+ nonselected equation vanishes in degree $\ell$ as well.
166
+
167
+ Continue inductively. A coefficient of degree $n$ can change only at
168
+ steps $n$ and $n+1$, so the resulting free series is well-defined.
169
+ Every fixed Schur coefficient is eventually zero and remains zero.
170
+ The construction also covers $g=0$, when the annihilator is zero.
171
+ For a periodic word the orbit consists of its distinct rotations; no
172
+ multiplicity is inserted into the annihilator calculation or into
173
+ \eqref{eq:correction-cyclic-input}.
174
+ \end{proof}
175
+
176
+ \begin{figure}[tbp]
177
+ \centering
178
+ \input{figures/eleven-block-offsets}
179
+ \caption{The eleven-block input pattern. Indices lie in $\mathbb Z/11\mathbb Z$.
180
+ The left panel shows the offset-one cycle; the right panel specifies all
181
+ four forward offsets, translated at every vertex. Each forward arrow carries a
182
+ generic pair of input matrices. At order $\ell\ge3$, a reverse correction
183
+ has degree $\ell-1$; degree-$\ell$ loop corrections are not drawn.}
184
+ \label{fig:eleven-blocks}
185
+ \end{figure}
186
+
187
+ Figure~\ref{fig:eleven-blocks} separates the generating cycle from the
188
+ full local arrow pattern. The role of the four offsets is now explicit. Avoiding returns of length
189
+ one or two starts the induction without changing the linear data.
190
+ Consecutive offsets within each color make its only obstructions
191
+ independent of the vertex. The remaining obstructions are exactly the
192
+ cyclic sums already proved to vanish.
193
+
194
+ \subsection{Fixed roots and Schur complements}
195
+
196
+ The following elementary fact identifies the spectral equations with a
197
+ single polynomial identity. Its coefficient ring need not be commutative.
198
+ Let $E$ be a field, let $\mathfrak a=(s_1,s_2)$ be the augmentation ideal
199
+ of the free algebra $E\langle s_1,s_2\rangle$, and put
200
+ \[
201
+ T_N=E\langle s_1,s_2\rangle/\mathfrak a^{N+1}
202
+ \qquad (N\geq 0).
203
+ \]
204
+ Elements of $E$ are central in $T_N$. Reduction modulo $\mathfrak a$
205
+ is called the constant term.
206
+
207
+ \begin{lemma}\label{lem:schur-polynomial}
208
+ Let $W\in M_d(T_N)$ have constant term
209
+ \[
210
+ W_0=\sum_{h=1}^{e}\lambda_h\pi_h,
211
+ \qquad
212
+ \pi_h\pi_j=\delta_{hj}\pi_h,
213
+ \qquad
214
+ \sum_{h=1}^{e}\pi_h=I_d,
215
+ \]
216
+ where the $\lambda_h\in E$ are distinct and the $\pi_h\in M_d(E)$
217
+ are nonzero projections. Set
218
+ \[
219
+ q(t)=\prod_{h=1}^{e}(t-\lambda_h),
220
+ \qquad \bar\pi_h=I_d-\pi_h.
221
+ \]
222
+ On the complementary summand $\bar\pi_h T_N^d$, the operator
223
+ \[
224
+ C_h=\bar\pi_h(W-\lambda_h I_d)\bar\pi_h
225
+ \]
226
+ is invertible. Define the Schur expression on $\pi_h T_N^d$ by
227
+ \[
228
+ S_h=\pi_h(W-\lambda_h I_d)\pi_h
229
+ -\pi_hW\bar\pi_h C_h^{-1}\bar\pi_hW\pi_h.
230
+ \]
231
+ Then $q(W)=0$ if and only if $S_h=0$ for every $h$.
232
+ \end{lemma}
233
+
234
+ \begin{proof}
235
+ The constant term of $C_h$ is
236
+ $\sum_{j\ne h}(\lambda_j-\lambda_h)\pi_j$, which is invertible on
237
+ $\bar\pi_h E^d$. A matrix over $T_N$ with invertible constant term is
238
+ invertible: after factoring out its constant term, the inverse is a
239
+ finite geometric series in a matrix with entries in $\mathfrak a$.
240
+ This proves the assertion about $C_h$. All modules below are right
241
+ $T_N$-modules, with matrices acting on column vectors from the left.
242
+
243
+ Suppose first that every $S_h$ vanishes. Define
244
+ $K_h:\pi_hT_N^d\longrightarrow T_N^d$ by
245
+ \[
246
+ K_hu=u-C_h^{-1}\bar\pi_hW\pi_hu,
247
+ \]
248
+ where the second term lies in the complementary summand. Then
249
+ $\pi_hK_hu=u$, and direct block multiplication gives
250
+ \[
251
+ (W-\lambda_h I_d)K_hu=S_hu=0.
252
+ \]
253
+ The map $K=\sum_hK_h\pi_h$ has constant term $I_d$, so it is
254
+ invertible. The displayed kernel equations imply
255
+ $WK=KW_0$. Consequently
256
+ \[
257
+ q(W)=Kq(W_0)K^{-1}=0.
258
+ \]
259
+
260
+ Conversely, suppose $q(W)=0$. Define
261
+ \[
262
+ P_h=\prod_{j\ne h}
263
+ \frac{W-\lambda_j I_d}{\lambda_h-\lambda_j}.
264
+ \]
265
+ These products are unambiguous because their factors are polynomials
266
+ in the same matrix with central scalar coefficients. Polynomial
267
+ interpolation modulo $q$ shows that the $P_h$ are spectral
268
+ idempotents; in particular,
269
+ \[
270
+ (W-\lambda_h I_d)P_h=0,
271
+ \qquad P_h\equiv\pi_h\pmod{\mathfrak a}.
272
+ \]
273
+ Let $\iota_h:\pi_hT_N^d\longrightarrow T_N^d$ be inclusion. The
274
+ endomorphism $A_h=\pi_hP_h\iota_h$ of $\pi_hT_N^d$ has constant
275
+ term the identity, and is therefore invertible. Thus
276
+ \[
277
+ \widetilde K_h=P_h\iota_hA_h^{-1}
278
+ \]
279
+ satisfies
280
+ $\pi_h\widetilde K_h=\operatorname{id}_{\pi_hT_N^d}$ and
281
+ $(W-\lambda_h I_d)\widetilde K_h=0$. The complementary component
282
+ of the latter equation determines its remaining component uniquely:
283
+ \[
284
+ \bar\pi_h\widetilde K_h
285
+ =-C_h^{-1}\bar\pi_hW\pi_h.
286
+ \]
287
+ Its $\pi_h$ component now gives $S_h=0$.
288
+ \end{proof}
289
+
290
+ For a matrix over $E\langle\!\langle s_1,s_2\rangle\!\rangle$,
291
+ apply Lemma~\ref{lem:schur-polynomial} after reduction to $T_N$.
292
+ It follows that the fixed-root Schur equations hold through degree
293
+ $N$ exactly when the identity $q(W)=0$ holds through degree $N$.
294
+ In particular, this equivalence applies at every finite stage of a
295
+ formal correction, with the same polynomial $q$ throughout.
preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/cyclic-obstruction.tex ADDED
@@ -0,0 +1,406 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Cyclic relations on the leading free-word errors}
2
+ \label{sec:cyclic-obstructions}
3
+
4
+ The space \(\mathcal G\) controls the linear corrections available
5
+ at several blocks. We must show that the errors to be corrected
6
+ satisfy its relations for individual cyclic orbits of free words.
7
+ Commuting scalar substitutions would combine too many words. We
8
+ instead substitute matrices, repeat each block, and attach hubs
9
+ whose derivative columns identify the possible left nullspace.
10
+
11
+ Traces of words and their cyclic symmetry are classical in matrix
12
+ invariant theory; see \cite[\S4]{Procesi1976}. Here the response
13
+ relations must first be proved to annihilate every matrix trace test.
14
+ An explicit directed-cycle calculation then isolates each cyclic orbit.
15
+
16
+ Fix \(m\geq1\) independent generic size-\(b\) points \(P_i\).
17
+ Write \(I_i\) for their selected root labels, so \(|I_i|=a\), and
18
+ let \(\mathcal G\subseteq\bigoplus_i H_{P_i}^*\) be the space
19
+ of Proposition~\ref{prop:compatible-relations}. As before, all
20
+ scalars may be extended to a common field containing the required
21
+ splitting data.
22
+
23
+ \begin{theorem}[Cyclic compatibility of the error]
24
+ \label{thm:cyclic-compatibility}
25
+ Let \(Z(s_1,s_2)\) be a pair of formal series in two free letters,
26
+ with constant term \(\operatorname{diag}(P_1,\ldots,P_m)\).
27
+ Suppose that the fixed-root Schur expressions \(S_{i,h}\), for
28
+ every block \(i\) and every root label \(h\), vanish in every
29
+ degree below \(\ell\), where \(\ell\geq1\).
30
+ By transfer, their degree-\(\ell\) coefficients are scalar on
31
+ their root spaces; write
32
+ \[
33
+ [s^\omega]S_{i,h}=e_{i,h,\omega}\pi_{i,h},
34
+ \qquad |\omega|=\ell.
35
+ \]
36
+ For each word the scalar tuple at block \(i\) belongs to its
37
+ active space. For every cyclic orbit \(\mathcal O\) of words of
38
+ length \(\ell\) and every \(c\in\mathcal G\),
39
+ \begin{equation}
40
+ \sum_{\omega\in\mathcal O}
41
+ \sum_{i=1}^m\sum_{h\in I_i}
42
+ c_{i,h}e_{i,h,\omega}=0.
43
+ \label{eq:cyclic-error-relation}
44
+ \end{equation}
45
+ The orbit sum runs over distinct words, including when a word has
46
+ a nontrivial rotational stabilizer.
47
+ \end{theorem}
48
+
49
+ We prove the theorem in three steps. First, arbitrary matrix
50
+ substitutions turn the free-word errors into matrices on a repeat
51
+ factor. Second, a derivative test shows that every relation in
52
+ \(\mathcal G\) annihilates their traces. Finally, directed-cycle
53
+ matrices isolate each cyclic orbit.
54
+
55
+ \begin{lemma}[Splitting repeated blocks]
56
+ \label{lem:repeated-splitting}
57
+ Fix \(L\geq1\) and arbitrary scalar matrices
58
+ \(S_1,S_2\in M_L(E)\). Substitute \(s_c=\delta S_c\) into
59
+ \(Z\), with a commuting Taylor parameter \(\delta\), and add
60
+ an order-\(\delta^\ell\) input loop \(Y_i\) in each old block
61
+ \(i\). Here \(Y_i\) is an arbitrary pair in
62
+ \(M_b(E)\otimes M_L(E)\). Put
63
+ \[
64
+ B_{i,h}=\sum_{|\omega|=\ell}
65
+ e_{i,h,\omega}S^\omega+D_{i,h}(Y_i),
66
+ \]
67
+ where \(D_{i,h}\) is applied entrywise to the repeat-factor
68
+ coefficients. One can choose the \(Y_i\) so that every \(B_{i,h}\),
69
+ for all root labels \(h\), has simple spectrum. For such a choice,
70
+ after a finite splitting extension the leaf output has branches
71
+ \[
72
+ \lambda_{i,h,j}(\delta)
73
+ =\lambda_{i,h}+\delta^\ell\theta_{i,h,j}
74
+ +O(\delta^{\ell+1}),\qquad 1\leq j\leq L,
75
+ \]
76
+ each scalar of multiplicity \(t\), where \(\theta_{i,h,j}\)
77
+ are the eigenvalues of \(B_{i,h}\). Their spectral projections
78
+ are integral in \(\delta\) and reduce to
79
+ \(\pi_{i,h}\otimes\Pi_{i,h,j}\), where
80
+ \(\Pi_{i,h,j}\) are the rank-one spectral projections of
81
+ \(B_{i,h}\).
82
+ \end{lemma}
83
+
84
+ \begin{proof}
85
+ Matrix substitution is legitimate coefficientwise in \(\delta\).
86
+ The leading Schur expression on the repeated \((i,h)\)-space is
87
+ \(I_t\otimes B_{i,h}\): the original errors give the first sum,
88
+ and an order-\(\delta^\ell\) input loop contributes its first
89
+ response. All lower orders are zero.
90
+
91
+ For each label \(h\), \(D_{i,h}\) is a nonzero linear functional
92
+ on the input directions. Its matrix-valued extension is therefore
93
+ onto \(M_L(E)\). The discriminant of \(B_{i,h}\), as a polynomial
94
+ in the loop coordinates, is consequently not identically zero.
95
+ There are finitely many labels, so the product of these discriminants
96
+ is nonzero. Over the infinite field in use, or a scalar extension,
97
+ choose loops at which their product is nonzero. This choice is made
98
+ for all labels, not merely the selected ones. For \(L=1\) the
99
+ simple-spectrum condition is automatic.
100
+
101
+ Separate the old distinct roots by a formal conjugation equal to
102
+ the identity at \(\delta=0\). The separated \((i,h)\)-block is
103
+ \begin{equation}
104
+ \lambda_{i,h}I+\delta^\ell(I_t\otimes B_{i,h})
105
+ +O(\delta^{\ell+1}).
106
+ \label{eq:old-cluster-expansion}
107
+ \end{equation}
108
+ Here is an exact comparison with the fixed-root Schur expression.
109
+ Write \(M=W-\lambda_{i,h}I\) in the fixed root/complement
110
+ decomposition, with blocks \(M_{uv}\). Its complementary block
111
+ \(M_{22}\) is invertible. If \(F\) is the separated root block
112
+ minus \(\lambda_{i,h}I\), its invariant columns can be written
113
+ \(\binom QR\), with \(Q=I+O(\delta)\), \(R=O(\delta)\), and
114
+ \(M\binom QR=\binom QR F\). Eliminating the lower row gives
115
+ \[
116
+ \bigl(M_{11}-M_{12}M_{22}^{-1}M_{21}\bigr)Q
117
+ =\bigl(Q-M_{12}M_{22}^{-1}R\bigr)F.
118
+ \]
119
+ The left parenthesis is the fixed-root Schur expression. Both
120
+ outer factors relating it to \(F\) reduce to identity at zero.
121
+ Consequently it and \(F\) have the same first nonzero coefficient.
122
+ Its vanishing below degree \(\ell\) forces the same vanishing
123
+ for \(F\), and its degree-\(\ell\) coefficient is
124
+ \(I_t\otimes B_{i,h}\). This proves
125
+ \eqref{eq:old-cluster-expansion}.
126
+
127
+ Within this block divide the change from \(\lambda_{i,h}I\) by
128
+ \(\delta^\ell\). Its constant term is \(I_t\otimes B_{i,h}\),
129
+ with \(L\) distinct eigenvalues. A second formal conjugation,
130
+ integral in \(\delta\), separates these slopes into blocks of
131
+ size \(t\). Across all old labels there are exactly
132
+ \[
133
+ mLe_b=e_{bmL}
134
+ \]
135
+ such blocks. Their characteristic polynomials are pairwise coprime
136
+ over the Laurent fraction field: different old roots are already
137
+ distinct at order zero, and distinct slopes separate the blocks
138
+ inside one old root. The minimal-degree bound at size \(bmL\)
139
+ is \(e_{bmL}\). Each separated block contributes at least one
140
+ to that degree, so each contributes exactly one and is scalar.
141
+ The two integral conjugations also give integral spectral
142
+ projections with the stated limits.
143
+ \end{proof}
144
+
145
+ Keep a choice as in Lemma~\ref{lem:repeated-splitting}. Adjoin
146
+ \(L+1\) independent generic size-\(b\) hub blocks, indexed by
147
+ \(p=1,\ldots,L\) and by \(*\), with spectra disjoint from the
148
+ old blocks. The individual hub \(p\) sends an input arrow to
149
+ repeat position \(p\) of every old block \(i\), with fixed generic
150
+ value \(U_{i,p}\). The common hub \(*\) sends the same generic
151
+ value \(U_{i,*}\) to every repeat position in old block \(i\).
152
+ There are no reverse arrows at this test input. Arrow values for
153
+ different pairs of old blocks and hubs can be chosen independently
154
+ and to satisfy the surjectivity conditions of
155
+ Lemma~\ref{lem:pair-quotient-surjectivity}.
156
+
157
+ Figure~\ref{fig:hub-test} shows the distinction between the individual
158
+ hubs and the common hub.
159
+
160
+ \begin{figure}[tbp]
161
+ \centering
162
+ \input{figures/repeated-leaves-hubs}
163
+ \caption{The hub test at $\delta=0$, for one old block $i$ and $L=3$.
164
+ Hub $p$ sends a generic matrix pair only to position $p$; the common hub
165
+ sends the same pair to all positions. Every old block uses these same
166
+ $L+1$ hubs. At $\delta\ne0$ the leaf input may couple repeat positions.
167
+ The individual hubs eliminate off-diagonal dual entries, and the common
168
+ hub identifies the diagonal functionals.}
169
+ \label{fig:hub-test}
170
+ \end{figure}
171
+
172
+ Treat the entire deformed leaf array as one block and order it
173
+ before the hubs. Over the \(\delta\)-Laurent field this is a star
174
+ with maximal root count. Put
175
+ \[
176
+ N=mL+L+1.
177
+ \]
178
+ Select the \(L\) branches over each old selected label and the
179
+ selected labels of all hubs, for a total of \(Na\) output rows.
180
+ The rank of their derivative matrix is at most
181
+ \(\rho_{bN}\leq Na-g\). This bound follows from the original
182
+ trace-minor identities, evaluated coefficientwise at the present
183
+ Taylor input; it does not require the specialized input to be
184
+ generic.
185
+
186
+ \newpage
187
+ \begin{lemma}[The limiting derivative columns]
188
+ \label{lem:limiting-columns}
189
+ The following derivative columns at the preceding star have finite
190
+ limits at \(\delta=0\).
191
+ \begin{enumerate}
192
+ \item A loop \(Y\otimes T\) inside old block \(i\) has limit
193
+ \[
194
+ D_{i,h}(Y)\operatorname{tr}(\Pi_{i,h,j}T)
195
+ \]
196
+ on row \((i,h,j)\), and zero on all other rows. Hub loops give
197
+ their own loop responses.
198
+ \item For individual hub \(p\), a reverse arrow of value \(V\)
199
+ from repeat position \(r\) in old block \(i\) has limit
200
+ \begin{align*}
201
+ &m_{i,h}(P_i,Q_p;U_{i,p},V)
202
+ \operatorname{tr}(\Pi_{i,h,j}E_{pr})
203
+ &&\text{on row }(i,h,j),\\
204
+ &\mathbf 1_{p=r}\,
205
+ m_{p,k}(Q_p,P_i;V,U_{i,p})
206
+ &&\text{on hub row }(p,k),
207
+ \end{align*}
208
+ and zero elsewhere. Here \(E_{pr}\) is the repeat-factor matrix
209
+ unit with row \(p\) and column \(r\).
210
+ \item For the common hub, use arrow \(U_{i,*}\) and replace the
211
+ repeat-factor matrix by
212
+ \[
213
+ \sum_{p=1}^L E_{pr}.
214
+ \]
215
+ The hub contribution is the single response
216
+ \(m_{*,k}(Q_*,P_i;V,U_{i,*})\).
217
+ \item The derivative along the whole input \(\delta\)-curve,
218
+ multiplied by \(\delta^{1-\ell}\), has limit
219
+ \(\ell\theta_{i,h,j}\) on leaf rows and zero on hub rows.
220
+ \end{enumerate}
221
+ The matrix consisting of a finite spanning collection of these
222
+ limiting columns has rank at most \(Na-g\).
223
+ \end{lemma}
224
+
225
+ \begin{proof}
226
+ Over the Laurent field, apply Lemma~\ref{lem:star-derivatives} with
227
+ the whole leaf array as one block. For loop derivatives, the
228
+ bounded leaf projection tends to
229
+ \(\pi_{i,h}\otimes\Pi_{i,h,j}\). Compression of the ordinary
230
+ first response gives \(D_{i,h}(Y)\) on the multiplicity space,
231
+ and taking trace divided by \(t\) gives the first formula.
232
+
233
+ For paired derivatives on a leaf, the Schur inverse is on the hub
234
+ at a root \(\lambda_{i,h,j}(\delta)\); that root stays away from
235
+ the hub spectrum at \(\delta=0\). For paired derivatives on a
236
+ hub, the inverse is on the leaf array at a hub root, which stays
237
+ away from every old leaf root. These inverses are regular at
238
+ \(\delta=0\). No inverse at the difference of two approaching
239
+ leaf roots occurs in this calculation.
240
+
241
+ At the reduction, the leaf input is diagonal between old blocks
242
+ and repeated inside each old block. A forward arrow at position
243
+ \(p\) followed by a reverse arrow from position \(r\) inserts
244
+ \(E_{pr}\) on the leaf repeat factor. At the hub end, the repeat
245
+ indices must match, giving \(\mathbf 1_{p=r}\). The ordinary
246
+ paired-response formula and trace divided by \(t\) now give the
247
+ second formula. Summing forward positions gives the common-hub
248
+ formula. The bounded projections and the distant-root inverses
249
+ justify all these limits coefficientwise.
250
+
251
+ The curve column lies in the span of input derivative columns over
252
+ the Laurent field by the chain rule. The expansion in
253
+ Lemma~\ref{lem:repeated-splitting} gives
254
+ \[
255
+ \delta^{1-\ell}\frac{d}{d\delta}
256
+ \lambda_{i,h,j}(\delta)
257
+ =\ell\theta_{i,h,j}+O(\delta).
258
+ \]
259
+ Hub roots are constant on the curve. Thus this column also has a
260
+ finite limit. Choose bases for the finitely many loop and reverse
261
+ direction spaces and include the curve column. Every
262
+ \((Na-g+1)\)-minor of the resulting matrix vanishes over the
263
+ Laurent field; since its entries have finite limits, these minors
264
+ remain zero after specialization. This proves the last assertion.
265
+ \end{proof}
266
+
267
+ We now use the individual hubs to remove off-diagonal repeat-factor
268
+ weights and the common hub to make all diagonal weights agree.
269
+ The rank bound will then show that no element of \(\mathcal G\)
270
+ has been lost.
271
+
272
+ \begin{lemma}[The left nullspace]
273
+ \label{lem:hub-nullspace}
274
+ The left nullspace of the limiting matrix in
275
+ Lemma~\ref{lem:limiting-columns}, including its curve column,
276
+ has dimension \(g\). Its projection to the old blocks identifies
277
+ it with \(\mathcal G\): for each \(c\in\mathcal G\), its leaf
278
+ weights are \(c_{i,h}\) on every row \((i,h,j)\), independently
279
+ of \(j\), and its hub weights are the uniquely determined
280
+ compatible functionals. Consequently
281
+ \begin{equation}
282
+ \sum_i\sum_{h\in I_i}c_{i,h}\operatorname{tr}(B_{i,h})=0
283
+ \qquad(c\in\mathcal G).
284
+ \label{eq:error-matrix-trace}
285
+ \end{equation}
286
+ \end{lemma}
287
+
288
+ \begin{proof}
289
+ Let \(\mu_{i,h,j}\) be leaf row weights in the left nullspace
290
+ and let \(\nu_p,\nu_*\) be the hub weights. Define
291
+ \[
292
+ T_{i,h}=\sum_{j=1}^L\mu_{i,h,j}\Pi_{i,h,j}\in M_L(E).
293
+ \]
294
+ The loop columns imply
295
+ \[
296
+ \sum_{h\in I_i}D_{i,h}(Y)
297
+ \operatorname{tr}(T_{i,h}T)=0
298
+ \qquad\text{for every }Y,T.
299
+ \]
300
+ Thus, for every matrix entry \((r,p)\), the coordinate vector
301
+ \( ((T_{i,h})_{rp})_{h\in I_i}\) defines a functional in
302
+ \(H_{P_i}^*\). The hub weights similarly belong to their own
303
+ loop annihilators.
304
+
305
+ Fix an individual hub \(p\) and a reverse position \(r\ne p\).
306
+ There is no hub response. Since
307
+ \[
308
+ \operatorname{tr}(T_{i,h}E_{pr})=(T_{i,h})_{rp},
309
+ \]
310
+ the reverse columns say that the functional with these
311
+ \((r,p)\)-entries kills the leaf endpoint projection of the paired
312
+ map. That projection is onto \(H_{P_i}\), so all these entries
313
+ vanish. As \(p,r\) vary, every \(T_{i,h}\) is diagonal. When
314
+ \(r=p\), the corresponding diagonal-entry functional and the
315
+ hub functional \(\nu_p\) are exactly a pair in the relation of
316
+ Proposition~\ref{prop:compatible-relations}.
317
+
318
+ For the common hub, the leaf expression is
319
+ \[
320
+ \operatorname{tr}\left(T_{i,h}\sum_pE_{pr}\right)
321
+ =\sum_p(T_{i,h})_{rp}=(T_{i,h})_{rr}.
322
+ \]
323
+ For every \(r\), this diagonal-entry functional is therefore
324
+ paired with the same \(\nu_*\). Projection of the pair relation
325
+ onto the hub dual space is an isomorphism, so the diagonal-entry
326
+ functionals are independent of \(r\). Compatibility for the
327
+ collection of old blocks and hubs identifies them across all old
328
+ blocks. Hence
329
+ \[
330
+ T_{i,h}=c_{i,h}I_L,
331
+ \qquad c\in\mathcal G,
332
+ \]
333
+ and all hub weights are uniquely determined by \(c\). Since the
334
+ rank-one projections \(\Pi_{i,h,j}\) are mutually orthogonal
335
+ and sum to identity, this also gives
336
+ \(\mu_{i,h,j}=c_{i,h}\). The map from the left nullspace to
337
+ \(\mathcal G\) is consequently injective.
338
+
339
+ There are \(Na\) rows, and the limiting rank is at most \(Na-g\)
340
+ even after the curve column is included. The nullspace therefore
341
+ has dimension at least \(g\). Its injection into the
342
+ \(g\)-dimensional space \(\mathcal G\) is an isomorphism.
343
+ In particular every \(c\in\mathcal G\), not just a possible
344
+ subspace of relations, occurs. Pairing its null vector with the
345
+ curve column and cancelling the nonzero integer \(\ell\) yields
346
+ \[
347
+ 0=\sum_i\sum_{h\in I_i}\sum_{j=1}^L
348
+ c_{i,h}\theta_{i,h,j}
349
+ =\sum_i\sum_{h\in I_i}c_{i,h}\operatorname{tr}(B_{i,h}).
350
+ \]
351
+ If \(g=0\), the same proof gives zero nullspace and the assertion
352
+ about \(c\) is vacuous. If \(L=1\), the off-diagonal step has
353
+ no entries to remove; the common-hub step still gives precisely
354
+ the stated conclusion.
355
+ \end{proof}
356
+
357
+ \begin{proof}[Proof of Theorem~\ref{thm:cyclic-compatibility}]
358
+ Apply Lemma~\ref{lem:hub-nullspace} to arbitrary \(S_1,S_2\)
359
+ and to the auxiliary loops chosen in
360
+ Lemma~\ref{lem:repeated-splitting}. The added-loop contribution
361
+ to \eqref{eq:error-matrix-trace} is zero. Indeed, write
362
+ \(Y_i=\sum_\alpha Y_{i,\alpha}\otimes T_{i,\alpha}\). Then
363
+ \[
364
+ \sum_{h\in I_i}c_{i,h}\operatorname{tr}(D_{i,h}(Y_i))
365
+ =\sum_\alpha\operatorname{tr}(T_{i,\alpha})
366
+ \sum_{h\in I_i}c_{i,h}D_{i,h}(Y_{i,\alpha})=0,
367
+ \]
368
+ because \(c_i\) annihilates the loop image. We conclude that,
369
+ for arbitrary matrix substitutions,
370
+ \begin{equation}
371
+ \sum_{|\omega|=\ell}
372
+ \left(\sum_i\sum_{h\in I_i}c_{i,h}e_{i,h,\omega}\right)
373
+ \operatorname{tr}(S^\omega)=0.
374
+ \label{eq:all-matrix-trace-tests}
375
+ \end{equation}
376
+ Auxiliary field extensions impose no restriction: this equality
377
+ has its coefficients in the original field, and extension is
378
+ injective.
379
+
380
+ We use a matrix-cycle test of the kind appearing in the constructive
381
+ trace argument of \cite[Proposition~4.1]{KlepSpenko2014}, recording the
382
+ rotational multiplicity explicitly. Fix a word
383
+ \(\omega_0=c_0c_1\cdots c_{\ell-1}\), with letters
384
+ \(c_j\in\{1,2\}\), and take \(L=\ell\). On vertices indexed
385
+ modulo \(\ell\), set
386
+ \[
387
+ S_c=\sum_{j:\,c_j=c}E_{j,j+1}\qquad(c=1,2).
388
+ \]
389
+ For a word \(\omega\) of length \(\ell\), its matrix trace
390
+ counts the starting vertices at which one reads \(\omega\)
391
+ around this directed cycle. It is zero unless \(\omega\) lies
392
+ in the cyclic orbit \(\mathcal O\) of \(\omega_0\); for every
393
+ distinct word in that orbit its value is the same positive integer
394
+ \[
395
+ \frac{\ell}{|\mathcal O|}.
396
+ \]
397
+ This is the rotational stabilizer size and includes periodic and
398
+ constant-letter words. Substitution into
399
+ \eqref{eq:all-matrix-trace-tests}, followed by cancellation of that
400
+ integer in characteristic zero, gives
401
+ \eqref{eq:cyclic-error-relation}.
402
+ \end{proof}
403
+
404
+ The leading errors now satisfy every cyclic relation imposed by
405
+ \(\mathcal G\). The colored correction graph will make these
406
+ exactly the annihilators of its order-by-order correction map.
preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/division-realization.tex ADDED
@@ -0,0 +1,240 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Realization in a central division algebra}
2
+ \label{sec:division-realization}
3
+
4
+ The preceding construction solved equations in split matrices. We now
5
+ place its constant blocks and prescribed arrows in one central division
6
+ algebra. Each subsequent correction is the solution of a finite linear
7
+ system over its center. This permits descent without any assertion that
8
+ solutions of nonlinear equations descend.
9
+
10
+ Throughout this section $k$ has characteristic zero and contains all roots
11
+ of unity, and $A$ is a central division algebra of degree $d$ over $k$.
12
+ The integer $b$ is the block size chosen earlier in the spectral case.
13
+ In the case where $q_0(w)=0$ already holds as a free-series identity, any
14
+ positive integer $b$ may be used. Put $m=11$.
15
+
16
+ \subsection{The two division-algebra factors}
17
+
18
+ Choose independent central indeterminates $\alpha,\beta$ and put
19
+ $k_0=k(\alpha,\beta)$. Let $B_b$ be the symbol algebra over $k_0$
20
+ generated by $u,v$ with
21
+ \[
22
+ u^b=\alpha,\qquad v^b=\beta,\qquad vu=\zeta_buv,
23
+ \]
24
+ where $\zeta_b$ is a primitive $b$-th root of unity. For $b=1$ this
25
+ means $B_1=k_0$. By the construction in Section~\ref{subsec:generic-division}, $B_b$
26
+ is central simple of degree $b$. Lemma~\ref{lem:symbol-division}
27
+ shows that $A\otimes_k B_b$ is division and remains division under
28
+ pure rational and central Laurent scalar extensions. We will use
29
+ these facts twice in adjoining the cyclic block factor.
30
+
31
+ Fix a $k_0$-basis $(e_a)_{a=1}^{b^2}$ of $B_b$. Over $k_0$ introduce
32
+ the following jointly independent variables:
33
+ \[
34
+ x_{c,a,j},\qquad y_{r,c,a,j},
35
+ \qquad
36
+ \begin{matrix}
37
+ c\in\{1,2\},\quad 1\le a\le b^2,\\
38
+ j\in\mathbb Z/m\mathbb Z,\quad r\in\{1,2,3,4\}.
39
+ \end{matrix}
40
+ \]
41
+ Let $L_0$ be their rational function field and let $\sigma$ increase
42
+ the index $j$ by one, fixing $k_0$. This automorphism has order exactly
43
+ $m$. Put $H_0=L_0^{\langle\sigma\rangle}$. Artin's fixed-field theorem
44
+ for a finite group of automorphisms gives a cyclic Galois extension
45
+ $L_0/H_0$ of degree $m$; see \cite[Corollary~3.11, p.~38]{MilneFT2022}.
46
+
47
+ Choose a further independent central indeterminate $a_*$ and form the
48
+ cyclic algebra $C$ over $F_0=H_0(a_*)$ with coefficient field
49
+ $L_0(a_*)$ and generator $\tau$, subject to
50
+ \begin{equation}
51
+ \tau^m=a_*,\qquad \tau c\tau^{-1}=\sigma(c)
52
+ \quad(c\in L_0).
53
+ \label{eq:cyclic-realization-relations}
54
+ \end{equation}
55
+ It has vector-space decomposition
56
+ $C=\bigoplus_{r=0}^{m-1}L_0(a_*)\tau^r$.
57
+ After extending scalars to a field containing $L_0(a_*)$, represent
58
+ $c\in L_0$ by the diagonal with entries $\sigma^{-i}(c)$ and
59
+ $\tau$ by the cyclic forward shift, whose wrap entry is $a_*$.
60
+ These matrices satisfy \eqref{eq:cyclic-realization-relations} and
61
+ span all matrix units. This gives the usual splitting of $C$ and
62
+ shows that it is central simple of degree $m$; see
63
+ \cite[Construction~2.5.1 and Proposition~2.5.2]{GilleSzamuely2006}.
64
+ Our conjugation convention uses the inverse of their Galois generator.
65
+
66
+ Define
67
+ \[
68
+ \widetilde B_0=(B_b\otimes_{k_0}F_0)\otimes_{F_0}C,
69
+ \qquad D_0=A\otimes_k\widetilde B_0.
70
+ \]
71
+ Then $D_0$ is central simple of degree $dbm$ over $F_0$ by the tensor-product and scalar-extension properties of
72
+ central simple algebras
73
+ \cite[Chapter~IV, Corollary~2.8 and Proposition~2.15]{MilneCFT}.
74
+ It is also division. Indeed
75
+ \[
76
+ D_L=(A\otimes_k B_b)\otimes_{k_0}L_0
77
+ \]
78
+ is division by the rational-extension argument. Extend $\sigma$ to
79
+ $D_L$ by fixing the old algebra factors. The skew Laurent division
80
+ ring $D_L((t;\sigma))$ receives a unital homomorphism from $D_0$
81
+ by $\tau\mapsto t$ and $a_*\mapsto t^m$. The central element
82
+ $t^m$ is transcendental over $H_0$. Simplicity again makes this map
83
+ injective, and finite dimension makes $D_0$ division.
84
+
85
+ Finally put
86
+ \[
87
+ F=F_0((\varepsilon)),\qquad
88
+ \widetilde B=\widetilde B_0\otimes_{F_0}F,\qquad
89
+ D=D_0\otimes_{F_0}F.
90
+ \]
91
+ The central Laurent argument shows that $D$ is a central division
92
+ algebra over $F$ of degree $dbm$. Input coefficients will lie in
93
+ $\widetilde B$, so that they commute with the old factor $A$.
94
+
95
+ \subsection{One realization of all generic data}
96
+
97
+ For $r\in\mathbb Z/m\mathbb Z$, let
98
+ \[
99
+ \mathcal V_r=
100
+ \bigl(B_b\otimes_{k_0}L_0\bigr)\tau^r
101
+ \otimes_{H_0}F
102
+ \ \subseteq\ \widetilde B.
103
+ \]
104
+ This notation uses the evident coefficient embedding and scalar
105
+ extension; equivalently it is the $F$-span of that graded summand in
106
+ $\widetilde B_0$. Upon splitting, $\mathcal V_r$ consists exactly
107
+ of all $b\times b$ entries at offset $r$ in the $m$-block matrix.
108
+ In fact $L_0\otimes_{H_0}E\simeq E^m$ over a splitting field $E$,
109
+ and $B_b$ becomes $M_b(E)$. Multiplication by $\tau^r$ moves these
110
+ independent diagonal entries to offset $r$, with nonzero wrap factors.
111
+ In particular $\mathcal V_0$ gives all diagonal blocks, and
112
+ $\mathcal V_{-r}$ gives all reverse entries for offset $r$.
113
+
114
+ Define the two constant inputs and four arrow pairs by
115
+ \[
116
+ P_c^0=\varepsilon\sum_a x_{c,a,0}e_a,
117
+ \qquad
118
+ U_{r,c}=\left(\sum_a y_{r,c,a,0}e_a\right)\tau^r
119
+ \quad(c=1,2).
120
+ \]
121
+ The prescribed initial substitution is the pair
122
+ \begin{equation}
123
+ Z_c^{\mathrm{init}}(s_1,s_2)
124
+ =P_c^0+(U_{1,c}+U_{2,c})s_1
125
+ +(U_{3,c}+U_{4,c})s_2.
126
+ \label{eq:division-initial-input}
127
+ \end{equation}
128
+ After splitting, the diagonal blocks of $(P_1^0,P_2^0)$ are exactly
129
+ the required independent small generic pairs. The two input-component
130
+ entries at every forward edge are independent generic entries, jointly
131
+ with all the diagonal data.
132
+
133
+ Here independence is over the old split coefficient field, which is the
134
+ field used in the generic rank tests. To check it, first split $A$ and
135
+ $B_b$ using constants independent of the variables $x,y$. The $m$
136
+ conjugates of each coefficient use the disjoint sets of variables with
137
+ different index $j$. The split symbol basis is a matrix basis.
138
+ Permuting those variables, changing that basis, and multiplying entries
139
+ by powers of $a_*$ preserve their algebraic independence. This verifies
140
+ all generic determinant conditions simultaneously. No independence
141
+ over the larger invariant field $H_0$ is asserted or needed.
142
+
143
+ We may perform the spectral calculations after extending $F$ to a
144
+ split Laurent field and then to the finite extensions needed for
145
+ eigenvalues. Its constant coefficient field contains the old algebraic
146
+ closure and the rational variables just chosen. The matrix constant
147
+ terms remain $\varepsilon$-small. Arrow coefficients need not be
148
+ small, since they occur only with positive free-word degree.
149
+
150
+ \subsection{Linear descent of the correction}
151
+
152
+ Assume first that $q_0(w)\ne0$. Let $W_0=w(P_1^0,P_2^0)\in D$
153
+ and choose its monic minimal polynomial
154
+ \begin{equation}
155
+ q(t)\in F[t].
156
+ \label{eq:fixed-central-polynomial}
157
+ \end{equation}
158
+ We keep this polynomial fixed throughout the correction. It is
159
+ irreducible, because $F[W_0]$ is a finite-dimensional commutative
160
+ domain, and separable because the characteristic is zero. In a
161
+ splitting field its roots are exactly the distinct eigenvalues of the
162
+ constant output. For completeness, left multiplication by $W_0$ on
163
+ $D$ has characteristic polynomial a power of $q$, since $D$ is a
164
+ vector space over $F[W_0]$. After splitting, that left multiplication
165
+ is a direct sum of copies of the action of the split matrix $W_0$.
166
+ Every root of $q$ therefore occurs in that matrix, and no other
167
+ eigenvalue occurs. Separability makes its action semisimple.
168
+
169
+ We solve $q(w(Z))=0$ in free series over $D$. Initially take
170
+ \eqref{eq:division-initial-input}. Its split Schur equations vanish
171
+ through degree two, so Lemma~\ref{lem:schur-polynomial} gives the same
172
+ assertion for the polynomial relation. Suppose inductively that a
173
+ partial substitution solves this relation through degree $\ell-1$,
174
+ where $\ell\ge3$. Allow a new coefficient in
175
+ $\mathcal V_{-r}^2$ at every word of length $\ell-1$, for
176
+ $r=1,2,3,4$, and a new coefficient in $\mathcal V_0^2$ at every word
177
+ of length $\ell$. These are finite-dimensional $F$-spaces.
178
+
179
+ Impose every coefficient equation of
180
+ \begin{equation}
181
+ q(w(Z))=0\pmod{(s_1,s_2)^{\ell+1}}.
182
+ \label{eq:finite-central-correction}
183
+ \end{equation}
184
+ This is a finite affine linear system over $F$ in the allowed new
185
+ coordinates. Indeed two new insertions have degree at least
186
+ $2(\ell-1)>\ell$. At any fixed free-word degree, only boundedly
187
+ many positive-degree insertions occur in the evaluation of the old
188
+ series; the remaining insertions are from the $\varepsilon$-small
189
+ constant input. The finitely many previously fixed coefficients have
190
+ a finite lower valuation bound. Thus the sums defining each
191
+ coefficient of \eqref{eq:finite-central-correction}, and its linear
192
+ part in the new coordinates, converge in $D$ and are defined over $F$.
193
+ Choosing an $F$-basis of $D$ turns them into finitely many ordinary
194
+ scalar linear equations.
195
+
196
+ After scalar extension, each permitted input space becomes exactly
197
+ the collection of reverse edges or loops used in
198
+ Proposition~\ref{prop:eleven-block-correction}. The current partial
199
+ substitution is a valid partial split solution by
200
+ Lemma~\ref{lem:schur-polynomial}. The proposition supplies a split
201
+ correction, and that lemma converts its Schur vanishings back to all
202
+ the equations in \eqref{eq:finite-central-correction}. In particular
203
+ the new degree-$\ell-1$ reverse coefficients preserve the already
204
+ solved equations: their diagonal Schur variation at that degree is
205
+ zero. We have therefore solved the whole finite linear system after
206
+ a field extension. A matrix and its augmented matrix have the same
207
+ ranks before and after extension, so the system already has a solution
208
+ over $F$.
209
+
210
+ Choose such a solution at every step. The coefficient stabilization
211
+ in Proposition~\ref{prop:eleven-block-correction} produces
212
+ \[
213
+ Z\in\widetilde B\langle\!\langle s_1,s_2\rangle\!\rangle^2,
214
+ \qquad q(w(Z))=0,
215
+ \]
216
+ with the prescribed constant and linear terms. Only finite linear
217
+ systems have been descended. Neither the roots of $q$ nor the split
218
+ correction coefficients need belong to $F$.
219
+
220
+ Since the input coefficients commute with $A$, evaluation at $Z$
221
+ defines a substitution homomorphism
222
+ \[
223
+ A\langle\!\langle z_1,z_2\rangle\!\rangle
224
+ \longrightarrow D\langle\!\langle s_1,s_2\rangle\!\rangle.
225
+ \]
226
+ It is well-defined by the same coefficientwise valuation bound: at
227
+ fixed output degree, only boundedly many nonconstant input factors
228
+ occur. The bound also justifies multiplication and regrouping of the
229
+ convergent coefficient sums. Hence every old polynomial identity on
230
+ the tuple and the chosen series is preserved by this substitution.
231
+
232
+ If $q_0(w)=0$ already holds, use the very same division algebra and
233
+ the initial substitution \eqref{eq:division-initial-input}, with any
234
+ $b\ge1$. No spectral correction is required; the old relation
235
+ $q_0(w)$ remains zero under the substitution homomorphism. Both cases
236
+ produce a central division algebra of degree $11bd>d$, with identical
237
+ generic forms for the constant and the two linear input coefficients.
238
+ The next step restores generation and two transverse directions using
239
+ these coefficients. That step is needed in the unconstrained case
240
+ as well as in the spectral case.
preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/formal-generic.tex ADDED
@@ -0,0 +1,406 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Formal evaluations and generic spectra}\label{sec:formal-generic}
2
+
3
+ We begin the proof of Theorem~\ref{thm:lifting} by constructing a
4
+ substitution $Z=(Z_1,Z_2)$ for the two free letters. Its coefficients will commute
5
+ with the old algebra $A$, so applying it to $(X,w)$ preserves their
6
+ polynomial identities. The matrix calculation focuses on $w$;
7
+ Sections~\ref{sec:division-realization} and~\ref{sec:generation}
8
+ realize the substitution in a division algebra of larger degree and
9
+ restore generation and both transverse directions for $X(Z)$.
10
+
11
+ Throughout the lifting argument, $k$ is a field of characteristic zero
12
+ containing all roots of unity, $A$ is a central division algebra of degree
13
+ $d$ over $k$, and
14
+ \[
15
+ w\in A\langle\!\langle z_1,z_2\rangle\!\rangle.
16
+ \]
17
+ The letters commute with $A$, but not with each other. Thus an element
18
+ is a family $(a_\omega)_\omega$ indexed by finite words, written
19
+ $\sum_\omega a_\omega z^\omega$, and multiplication uses concatenation
20
+ of words. Fix an algebraic closure $K$ of $k$ and a splitting
21
+ $A\otimes_k K\simeq M_d(K)$; this uses the splitting and
22
+ scalar-extension properties of central simple algebras
23
+ \cite[Chapter~IV, Example~2.14(a) and Proposition~2.15]{MilneCFT}.
24
+
25
+ If $P=(P_1,P_2)$ is a pair of $n\times n$ indeterminate matrices, put
26
+ \[
27
+ W_n(P)=\sum_\omega a_\omega\otimes P^\omega
28
+ \in M_{dn}(K[[P]]).
29
+ \]
30
+ Here $K[[P]]$ is the ordinary commutative power series ring in the
31
+ $2n^2$ entries. We omit the subscript $n$ when the size is clear.
32
+ The coefficient matrices act on the first tensor factor. In
33
+ particular, every input arrow between blocks is a pair of scalar
34
+ matrices acting on the second factor. It is not an arbitrary pair of
35
+ matrices on both factors.
36
+
37
+ In the spectral case we seek a substitution $Z=(Z_1,Z_2)$, with
38
+ constant term $R$, for which $W(Z)$ is conjugate to a split semisimple
39
+ constant output $W(R)$. If $\Lambda$ is the set of distinct eigenvalues
40
+ of $W(R)$, this gives
41
+ \[
42
+ q(W(Z))=0,\qquad q(t)=\prod_{\lambda\in\Lambda}(t-\lambda).
43
+ \]
44
+ The division realization will identify $q$ with the minimal polynomial
45
+ over its central coefficient field. If $w$ already satisfies the
46
+ minimal polynomial of $w(0)$, substitution retains that relation and
47
+ the spectral correction is unnecessary.
48
+
49
+ For the spectral construction, we will find matrix sizes with a common
50
+ eigenvalue multiplicity, disjoint spectra at independent inputs, and
51
+ scalar spectral blocks under commuting Taylor perturbations. These
52
+ properties will make the eigenvalue responses of
53
+ Section~\ref{sec:responses} well-defined. We first specify the
54
+ evaluations and specializations used to establish them and to evaluate
55
+ triangular auxiliary inputs later.
56
+
57
+ \subsection{Convergence and specialization}\label{subsec:formal-conventions}
58
+
59
+ Let $E$ be a complete discretely valued field containing $K$, with
60
+ valuation $v$, such that $v(c)=0$ for $c\in K^\times$. We use
61
+ $E=C((\varepsilon))$, or a finite extension of such a field, and
62
+ normalize $v(\varepsilon)=1$. Matrix valuations mean the minimum of
63
+ the entry valuations. A matrix is \emph{small} if this minimum is
64
+ positive. A small generic point is
65
+ $P=\varepsilon P^\circ$, where all entries of $P^\circ$ are
66
+ algebraically independent over the previously specified constant
67
+ field. Several independent points can use the same $\varepsilon$.
68
+
69
+ The finite extensions used to split spectra are separable in
70
+ characteristic zero. The valuation extends to each such extension,
71
+ which remains complete and discretely valued
72
+ \cite[Theorem~7.38 and Remark~7.43]{MilneANT}; with the normalization
73
+ $v(\varepsilon)=1$, its value group may be $\frac1e\mathbb Z$ for a
74
+ positive integer $e$.
75
+
76
+ \begin{lemma}[Admissible evaluations]\label{lem:admissible-evaluation}
77
+ Suppose a constant input pair $R$ is block upper triangular with $b$
78
+ blocks and small diagonal blocks. Its strictly upper blocks may have
79
+ arbitrary entries in $E$. Let $H$ be a matrix pair of formal series
80
+ of positive order in finitely many commuting or free variables.
81
+ Then $W(R+H)$ is defined coefficientwise by convergent sums in $E$.
82
+ The same assertion holds for products, finite determinants, and
83
+ derivatives of fixed order of finitely many such entry series.
84
+
85
+ These evaluations preserve formal entry identities. They also
86
+ remain valid coefficientwise in an additional parameter $\eta$ if
87
+ the diagonal blocks have entries in $E[[\eta]]$ with small constant
88
+ terms, while the strictly upper blocks and the coefficients of $H$
89
+ have entries in $E((\eta))$.
90
+ \end{lemma}
91
+
92
+ \begin{proof}
93
+ Fix a coefficient of degree $r$ in the variables of $H$. An input
94
+ path contributing to this coefficient uses at most $r$ positive-order
95
+ terms of $H$. Between these insertions it follows the constant upper
96
+ triangular pair. In each of the at most $r+1$ resulting intervals,
97
+ there are at most $b-1$ strictly upper steps. Thus at most
98
+ $(r+1)(b-1)$ constant factors are strictly upper. All remaining
99
+ constant factors come from small diagonal blocks.
100
+
101
+ Only finitely many coefficients of $H$ can occur at the chosen degree.
102
+ Their valuations, and those of the finitely many strictly upper
103
+ blocks, have a common lower bound. If the original word has length
104
+ $L$, its contribution consequently has valuation at least
105
+ $cL-C_r$, where $c>0$ and $C_r$ is independent of the word. There
106
+ are finitely many words of each length, so the sum converges. The
107
+ same estimate applies after inserting the finitely many extra factors
108
+ needed for a product or a derivative of fixed order. Completeness
109
+ allows regrouping of these sums, proving compatibility with
110
+ multiplication and with identities.
111
+
112
+ For the last assertion, first fix both the degree $r$ in $H$ and an
113
+ $\eta$-coefficient. The bounded number of strictly upper steps and
114
+ of $H$-insertions bounds their total negative $\eta$-order. Hence
115
+ only a bounded number of positive-order diagonal $\eta$-terms can
116
+ contribute, and only finitely many of their coefficients are used.
117
+ Every other factor is a small constant diagonal term. The preceding
118
+ valuation estimate therefore applies again. The resulting assertion
119
+ is coefficientwise; no interchange of the two Laurent topologies is
120
+ being asserted.
121
+ \end{proof}
122
+
123
+ We will use inverses of finite matrices as rational operations after
124
+ evaluation. The following elementary distinction is important.
125
+ Although $(\varepsilon-Q)^{-1}$ has a formal expansion at $Q=0$ over
126
+ $E$, that expansion need not converge after $Q=\varepsilon Q^\circ$.
127
+ Accordingly, when transferring an identity involving an inverse, we
128
+ first multiply by its determinant. We evaluate the resulting
129
+ numerator by Lemma~\ref{lem:admissible-evaluation}, and divide only
130
+ when the evaluated determinant is nonzero. Formal inverse expansions
131
+ are used to define coefficients; they are not presumed to converge at
132
+ every subsequent specialization.
133
+
134
+ \begin{lemma}[Detection by independent residues]\label{lem:generic-detection}
135
+ Let
136
+ \[
137
+ F(Q)=\sum_\alpha c_\alpha Q^\alpha\in E[[Q_1,\ldots,Q_N]],
138
+ \qquad \inf_\alpha v(c_\alpha)>-\infty.
139
+ \]
140
+ Adjoin elements $Q_1^\circ,\ldots,Q_N^\circ$ whose residues are
141
+ algebraically independent over the residue field of $E$, and complete
142
+ with respect to the extended valuation. Then
143
+ $F(\varepsilon Q^\circ)$ is defined, and is nonzero whenever $F$ is
144
+ nonzero.
145
+ \end{lemma}
146
+
147
+ \begin{proof}
148
+ The valuations $v(c_\alpha)+|\alpha|$ tend uniformly to infinity
149
+ with $|\alpha|$. Their least value is therefore attained by a
150
+ nonempty finite set of monomials. After scaling to this valuation,
151
+ the residue of their sum is a nonzero polynomial in the independent
152
+ residues of the $Q_j^\circ$. This proves both assertions.
153
+ \end{proof}
154
+
155
+ In applications, the coefficients of a cleared numerator are finite
156
+ sums of products of base-point scalars and matrix-entry series.
157
+ The path estimate gives a uniform valuation bound in the auxiliary
158
+ coordinates. Lemma~\ref{lem:generic-detection} therefore identifies
159
+ formal identities in these coordinates with identities at independent
160
+ small generic points. The base-point valued field is constructed
161
+ first; the auxiliary residues are adjoined afterward. This order
162
+ keeps their independence valid even after the base spectrum has been
163
+ split. The argument can be applied separately at each Taylor degree.
164
+
165
+ We record two further field conventions. Evaluation
166
+ \[
167
+ K[[P]]\longrightarrow C(P^\circ)((\varepsilon)),
168
+ \qquad P\longmapsto\varepsilon P^\circ,
169
+ \]
170
+ is injective, by homogeneous degree or by
171
+ Lemma~\ref{lem:generic-detection}. It extends to the fraction field,
172
+ and a finite splitting field embeds into a finite algebraic extension
173
+ of the target. Also, if $R$ is a small constant pair, then
174
+ \begin{equation}
175
+ K[[P]]\longrightarrow E[[\Delta]],\qquad P\longmapsto R+\Delta
176
+ \label{eq:generic-taylor-embedding}
177
+ \end{equation}
178
+ is injective: reduction modulo the valuation ideal sends the image of
179
+ $f$ to $f(\Delta)$. We use this observation for small block diagonal
180
+ $R$. Denominators in the fraction field remain nonzero, so the map
181
+ extends to fraction fields.
182
+
183
+ Finally, the Taylor substitution $P\mapsto P+\eta v$ maps
184
+ $\operatorname{Frac}K[[P]]$ into
185
+ $\operatorname{Frac}K[[P]][[\eta]]$, with reduction the identity.
186
+ It extends to a finite separable extension $\Omega$ with values in
187
+ $\Omega[[\eta]]$: choose a primitive element and lift its defining
188
+ equation using its nonzero derivative. The lift reducing to the
189
+ chosen primitive element is unique, by coefficient recursion. This
190
+ convention lets us move a base point while retaining its labeled
191
+ eigenvalue branches.
192
+
193
+ \subsection{Generic division evaluations}\label{subsec:generic-division}
194
+
195
+ Generic matrix evaluations have a useful divisibility property for
196
+ their eigenvalue multiplicities. We obtain it by first evaluating
197
+ inside a division algebra.
198
+
199
+ For $n\ge1$, choose independent central variables $\alpha,\beta$
200
+ and a primitive $n$th root of unity $\zeta_n\in k$. Over
201
+ $k_0=k(\alpha,\beta)$ let $B_n$ be generated by $x,y$ with
202
+ \[
203
+ x^n=\alpha,\qquad y^n=\beta,\qquad yx=\zeta_nxy.
204
+ \]
205
+ For $n=1$ this means $B_1=k_0$. The reduced monomials
206
+ $x^iy^j$, $0\le i,j<n$, form a basis. Indeed they span by the
207
+ relations, and after adjoining $n$th roots of $\alpha$ and $\beta$
208
+ their clock-and-shift matrices are linearly independent. These
209
+ matrices span $M_n$, so $B_n$ is central simple of degree $n$.
210
+ This is the standard symbol construction
211
+ \cite[Corollary~2.5.5(1)]{GilleSzamuely2006}, with the inverse
212
+ root of unity for our convention.
213
+
214
+ \begin{lemma}\label{lem:symbol-division}
215
+ The central simple algebra $A\otimes_k B_n$ is division. Its pure
216
+ rational scalar extensions and its central Laurent series extensions
217
+ are division as well.
218
+ \end{lemma}
219
+
220
+ \begin{proof}
221
+ Start with $A((x))$, where $x$ commutes with $A$, and let $\sigma$
222
+ fix $A$ and send $x$ to $\zeta_nx$. The skew Laurent series ring
223
+ $A((x))((y;\sigma))$, with $ya=\sigma(a)y$, is a division ring by
224
+ the leading-coefficient construction of inverses. The elements
225
+ $x^n,y^n$ are central and algebraically independent. The defining
226
+ relations give a unital map of $A\otimes_k B_n$ into this division
227
+ ring. Central simplicity makes the map injective. A finite
228
+ dimensional domain over a field is division, since multiplication by
229
+ a nonzero element is an injective and hence surjective linear map.
230
+
231
+ For a central division algebra $D/F$, the rational extension $D(t)$
232
+ embeds in the division ring $D((t))$. Iterating proves the rational
233
+ assertion. Because $D$ has a finite $F$-basis,
234
+ $D\otimes_F F((\varepsilon))=D((\varepsilon))$, which is again
235
+ division by leading coefficients.
236
+ \end{proof}
237
+
238
+ Choose a basis $b_1,\ldots,b_{n^2}$ of $B_n$, and let
239
+ $c_{ij}$, $i=1,2$, $j=1,\ldots,n^2$, be independent variables.
240
+ Evaluate $w$ at
241
+ \[
242
+ P_i=\varepsilon\sum_j c_{ij}b_j.
243
+ \]
244
+ This gives an element of a central division algebra of degree $dn$
245
+ over
246
+ \[
247
+ F_n=k(\alpha,\beta,(c_{ij}))((\varepsilon)).
248
+ \]
249
+ After splitting $A$ and $B_n$ by constants independent of the $c_{ij}$,
250
+ the $b_j$ become a basis of $M_n$. The change from the $c_{ij}$ to
251
+ the entries of $P_i/\varepsilon$ is therefore an invertible linear
252
+ change of independent coordinates. The resulting evaluation is a
253
+ small generic scalar matrix evaluation in the sense fixed above.
254
+
255
+ Let $e_n$ denote the minimal-polynomial degree of this element. Its
256
+ minimal polynomial is irreducible and separable over $F_n$.
257
+ Consequently $W(P)$ is semisimple over a splitting field, and every
258
+ distinct root has the same multiplicity
259
+ \begin{equation}
260
+ t_n=\frac{dn}{e_n}.
261
+ \label{eq:generic-multiplicity}
262
+ \end{equation}
263
+ For completeness, if $D/F$ has degree $N$ and $a\in D$ has minimal
264
+ polynomial $q$ of degree $e$, then left multiplication by $a$ has
265
+ characteristic polynomial $q^{N^2/e}$: view $D$ as a vector space
266
+ over $F[a]$. After splitting $D=M_N$, left multiplication acts by
267
+ the matrix $a$ on each of its $N$ columns. Its characteristic
268
+ polynomial is therefore the $N$th power of the matrix characteristic
269
+ polynomial. Comparing root multiplicities gives $N/e$ in the
270
+ matrix representation. This also proves that $N/e$ is an integer.
271
+
272
+ Linear independence of $1,a,\ldots,a^{e-1}$ is preserved by field
273
+ extension. Thus the same $e_n,t_n$ describe $W(P)$ over a splitting
274
+ field of $\operatorname{Frac}K[[P]]$.
275
+
276
+ \subsection{Nonconstant roots and stable multiplicity}
277
+ \label{subsec:stable-multiplicity}
278
+
279
+ Let $q_0$ be the minimal polynomial of $w(0)$ over $k$. If
280
+ $q_0(w)=0$ as a free series, the subsequent spectral construction is
281
+ unnecessary; the unconstrained case of the lifting argument will use
282
+ this existing relation. In the rest of this section assume
283
+ $q_0(w)\ne0$.
284
+
285
+ A nonzero homogeneous part of $q_0(w)$ is detected by scalar matrices
286
+ of every sufficiently large size. To see this, choose a word of
287
+ length $L$ with nonzero coefficient and use a path of $L+1$ vertices,
288
+ placing its successive letters on the consecutive matrix-unit
289
+ arrows. The $(1,L+1)$ entry detects precisely that coefficient.
290
+ Padding by zero blocks works for all larger sizes. It follows that
291
+ $q_0(W(P))\ne0$ at every generic size $n\ge n_0$, for some $n_0$.
292
+
293
+ \begin{lemma}\label{lem:nonconstant-roots}
294
+ For $n\ge n_0$, every distinct generic eigenvalue of $W(P)$ has a
295
+ nonzero differential in the input entries. Independent small generic
296
+ points of sizes at least $n_0$ have disjoint spectra. Their spectra
297
+ also avoid the constant spectrum of $w(0)$.
298
+ \end{lemma}
299
+
300
+ \begin{proof}
301
+ Use the division evaluation over $F_n$. Each derivation
302
+ $\partial/\partial c_{ij}$ acts coefficientwise on Laurent series
303
+ and extends uniquely to algebraic extensions in characteristic zero.
304
+ Uniqueness implies that it commutes with automorphisms of a splitting
305
+ field over $F_n$. If all these derivations killed one root, they
306
+ would kill all its Galois conjugates. Irreducibility makes these all
307
+ the distinct roots. Thus every coefficient of the reduced
308
+ characteristic polynomial would have all its input derivatives zero.
309
+
310
+ The coefficient of $\varepsilon^r$ in such a characteristic
311
+ coefficient is a homogeneous polynomial of degree $r$ in the
312
+ $c_{ij}$. In characteristic zero a polynomial whose partial
313
+ derivatives all vanish is constant. All terms of positive
314
+ $\varepsilon$-degree therefore vanish. The characteristic polynomial
315
+ is the characteristic polynomial of $w(0)$. Semisimplicity then
316
+ implies $q_0(W(P))=0$, a contradiction.
317
+
318
+ Splitting $A,B_n$ uses constants independent of the inputs. The
319
+ invertible basis change described above, together with the nonzero
320
+ factor $\varepsilon$, transports the differential assertion to
321
+ ordinary matrix-entry coordinates. For independent points $P,Q$,
322
+ derivations in the $P$-coordinates kill the roots belonging to $Q$.
323
+ They cannot kill a root belonging to $P$. No root can therefore
324
+ belong to both spectra. The same argument excludes a constant root.
325
+ \end{proof}
326
+
327
+ Choose $p\ge n_0$ for which the positive integer $t_p$ is minimal
328
+ among all $t_n$, $n\ge n_0$, and put
329
+ \[
330
+ t=t_p,\qquad \mathcal S=\{pN:N\ge1\}.
331
+ \]
332
+
333
+ \begin{lemma}\label{lem:stable-multiplicity}
334
+ For every $N\ge1$,
335
+ \[
336
+ t_{pN}=t,\qquad e_{pN}=Ne_p.
337
+ \]
338
+ \end{lemma}
339
+
340
+ \begin{proof}
341
+ Specialize a size-$pN$ point to a diagonal sum of $N$ independent
342
+ size-$p$ points. Lemma~\ref{lem:nonconstant-roots} gives $Ne_p$
343
+ distinct eigenvalues there. The generic bound on minimal-polynomial
344
+ degree survives this specialization: it is expressed by the vanishing
345
+ of all $(e_{pN}+1)$-minors of the matrix whose columns are the
346
+ vectorizations of $1,W,\ldots,W^{e_{pN}}$. These are formal entry
347
+ identities covered by Lemma~\ref{lem:admissible-evaluation}.
348
+ Consequently $e_{pN}\ge Ne_p$. Minimality of $t$ gives the opposite
349
+ inequality,
350
+ $e_{pN}=dpN/t_{pN}\le dpN/t=Ne_p$.
351
+ \end{proof}
352
+
353
+ We henceforth use sizes in $\mathcal S$. At size $n$, the minimal
354
+ polynomial always has degree at most $e_n=dn/t$ at every admissible
355
+ specialization. The following consequence controls all commuting
356
+ Taylor deformations used below.
357
+
358
+ \begin{lemma}[Scalar branches at maximal root count]
359
+ \label{lem:scalar-branches}
360
+ Let $V(T)$ be a matrix over a commuting formal Taylor ring $E[[T]]$.
361
+ Suppose $V(0)$ is split semisimple with $e$ distinct eigenvalues and
362
+ the minimal-polynomial degree of $V(T)$ over
363
+ $\operatorname{Frac}E[[T]]$ is at most $e$. Then a formal change of
364
+ basis reducing to the identity separates $V(T)$ into $e$ scalar
365
+ blocks. The sizes of these blocks are their multiplicities at
366
+ $T=0$.
367
+ \end{lemma}
368
+
369
+ \begin{proof}
370
+ Use the eigenspace decomposition at zero. Off-diagonal blocks can be
371
+ removed recursively in total Taylor degree: the equation for the
372
+ block between eigenvalues $\lambda_i,\lambda_j$ is multiplication
373
+ by $\lambda_i-\lambda_j$, a nonzero scalar. We obtain blocks
374
+ $V_i(T)$ reducing to $\lambda_i I$. Their characteristic polynomials
375
+ have pairwise unit resultants, because their reductions have different
376
+ roots. Their minimal polynomials over the Taylor fraction field are
377
+ therefore pairwise coprime. The minimal-polynomial degree of their
378
+ direct sum is the sum of their degrees. There are $e$ nonempty
379
+ blocks and the total degree is at most $e$, so every block has
380
+ minimal-polynomial degree one. Each $V_i(T)$ is scalar. Its scalar
381
+ entry belongs to $E[[T]]$, since the block entries do.
382
+ \end{proof}
383
+
384
+ In particular, the roots at a small semisimple point with $e_n$
385
+ distinct roots have labeled scalar Taylor branches. The splitting
386
+ field of the generic point embeds in their Taylor fraction field by
387
+ \eqref{eq:generic-taylor-embedding}; a labeling is chosen by reduction
388
+ to the roots at the base.
389
+
390
+ Let $\rho_n$ be the generic rank of the input Jacobian of
391
+ \[
392
+ \operatorname{tr}W,\operatorname{tr}W^2,\ldots,
393
+ \operatorname{tr}W^{dn}.
394
+ \]
395
+ Its minors are formal entry identities, so $\rho_n$ bounds the
396
+ corresponding specialized ranks. At a maximal-root-count point the
397
+ scalar branches satisfy
398
+ \[
399
+ d\operatorname{tr}W^j
400
+ =jt\sum_{h=1}^{e_n}\lambda_h^{j-1}\,d\lambda_h.
401
+ \]
402
+ The first $e_n$ rows give an invertible Vandermonde matrix. Hence
403
+ the trace Jacobian and the eigenvalue Jacobian have the same rank
404
+ there, including over a commuting Taylor fraction field. We have
405
+ therefore obtained both ingredients needed for the response
406
+ calculations: scalar branches and specialization-stable rank bounds.
preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/generation.tex ADDED
@@ -0,0 +1,310 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Restoring generation and two transverse directions}
2
+ \label{sec:generation}
3
+
4
+ The preceding construction gives a substitution $Z(s_1,s_2)$ inside
5
+ the centralizer of $A$ in a larger central division algebra. It
6
+ preserves the old polynomial identities and algebraizes the chosen
7
+ series. To complete Theorem~\ref{thm:lifting}, we must
8
+ make the new constant tuple generate the larger algebra and retain
9
+ two independent directions modulo inner derivations. We first use the
10
+ original transverse directions to prove generation of the generic
11
+ diagonal product and to control the arrows between its blocks.
12
+ Translating the first free letter by a new central parameter then joins
13
+ the blocks into a full matrix algebra. A single rank calculation shows
14
+ that both directions remain independent modulo inner derivations.
15
+
16
+ Throughout this section, brackets with a tuple are taken componentwise.
17
+ Thus, for $C=(C_1,\ldots,C_u)$ in an algebra $B$, write
18
+ \[
19
+ J(C)=\{([T,C_1],\ldots,[T,C_u]):T\in B\}.
20
+ \]
21
+ Polynomial relations on $X_0$ detect the two input directions to first
22
+ order.
23
+
24
+ \begin{lemma}[Derivatives of relations]
25
+ \label{lem:derivatives-of-relations}
26
+ Let $A$ be a finite-dimensional central simple algebra over a field
27
+ $k$ of characteristic zero. Let
28
+ $X\in A\langle\!\langle z_1,z_2\rangle\!\rangle^u$ have constant
29
+ tuple $X_0$ generating $A$, and suppose its two linear coefficients
30
+ $X_1,X_2$ are independent modulo $J(X_0)$. Define
31
+ \[
32
+ \theta:k\langle x_1,\ldots,x_u\rangle\longrightarrow A,
33
+ \qquad \theta(f)=f(X_0),\qquad I=\ker\theta.
34
+ \]
35
+ Then the map taking $f\in I$ to the coefficients of $z_1,z_2$ in
36
+ $f(X)$ is onto $A^2$.
37
+ \end{lemma}
38
+
39
+ \begin{proof}
40
+ Denote these two coefficient maps by $\delta_1,\delta_2$. Each
41
+ satisfies
42
+ \[
43
+ \delta_j(fg)=\theta(f)\delta_j(g)+\delta_j(f)\theta(g).
44
+ \]
45
+ Since $\theta$ is onto and $I$ is a two-sided ideal, the image
46
+ $M=(\delta_1,\delta_2)(I)$ is an $A$-bimodule in $A^2$.
47
+
48
+ Left and right multiplication generate $\operatorname{End}_k(A)$;
49
+ see \cite[Chapter~IV, Corollary~2.9]{MilneCFT}.
50
+ Indeed, after splitting $A$, multiplication by matrix units on the
51
+ left and right gives every matrix unit on the vector space $A$;
52
+ the resulting isomorphism
53
+ $A\otimes_k A^{\mathrm{op}}\simeq\operatorname{End}_k(A)$ descends
54
+ by finite-dimensional linear algebra. Applying these endomorphism
55
+ matrix units to $M\subseteq A\otimes_k k^2$ shows that
56
+ $M=A\otimes_k V$ for a subspace $V\subseteq k^2$.
57
+ If $V\ne k^2$, some nonzero $(a,b)\in k^2$ annihilates $V$.
58
+ The map $a\delta_1+b\delta_2$ then vanishes on $I$ and descends to
59
+ a derivation of $A$.
60
+
61
+ Every $k$-linear derivation of $A$ is inner
62
+ \cite[Theorem~8]{Jacobson1937Derivations}. For completeness, after
63
+ splitting $A=M_d(E)$, a derivation $\partial$ is implemented by
64
+ \[
65
+ T=\sum_i\partial(E_{i1})E_{1i}.
66
+ \]
67
+ Differentiating $E_{kl}E_{i1}=\delta_{li}E_{k1}$, multiplying by
68
+ $E_{1i}$, and summing gives $\partial(E_{kl})=[T,E_{kl}]$.
69
+ The equations for an implementing element on a fixed $k$-basis of
70
+ $A$ form a linear system over $k$. Solvability after scalar
71
+ extension implies solvability over $k$.
72
+ It follows that $aX_1+bX_2\in J(X_0)$, a contradiction.
73
+ \end{proof}
74
+
75
+ In particular, there are $f_1,f_2\in I$ whose derivative pairs are
76
+ $(1,0)$ and $(0,1)$. These relations recover the two generic input
77
+ matrices from small evaluations of the tuple.
78
+
79
+ \begin{lemma}[Generic blocks]
80
+ \label{lem:generic-generating-blocks}
81
+ Under the hypotheses of Lemma~\ref{lem:derivatives-of-relations},
82
+ write $d=\deg A$ and split $A$ into $d\times d$ matrices. Fix a
83
+ positive integer $b$ and finitely many independent small generic input pairs
84
+ \[
85
+ P_i=\varepsilon P_i^{\circ},\qquad 1\le i\le r,
86
+ \]
87
+ of $b\times b$ matrices, with jointly independent entries in the
88
+ $P_i^{\circ}$. Work over a common splitting Laurent field.
89
+ Then each tuple $C_i=X(P_i)$ generates $M_{db}$, and the diagonal
90
+ tuple $C=\operatorname{diag}(C_i)$ generates the full product of
91
+ these matrix algebras.
92
+
93
+ For distinct $i,j$, the output derivative of a generic input arrow
94
+ $U=(U_1,U_2)$ from block $j$ to block $i$ is nonzero modulo
95
+ \[
96
+ \{C_iT-TC_j:T\in M_{db}\}.
97
+ \]
98
+ More precisely, the image of the arrow derivatives in this quotient
99
+ has dimension at least $b^2$.
100
+ \end{lemma}
101
+
102
+ \begin{proof}
103
+ Let $E$ contain the splitting data and independent input coordinates.
104
+ Consider integral elements of the $E((\varepsilon))$-algebra
105
+ generated by $X(P_i)$. Their reductions modulo $\varepsilon$
106
+ contain $M_d(E)\otimes1$, because $X_0$ generates the old algebra.
107
+ Lemma~\ref{lem:derivatives-of-relations} also gives
108
+ \[
109
+ \varepsilon^{-1}f_j(X(P_i))
110
+ \equiv I_d\otimes P_{i,j}^{\circ}\pmod\varepsilon.
111
+ \]
112
+ A generic pair generates $M_b(E)$. To see the relevant determinant
113
+ is nonzero, specialize one matrix to a diagonal matrix with distinct
114
+ entries and the other to a matrix with every entry nonzero.
115
+ Interpolation and sandwiching give all matrix units. Thus the
116
+ reductions generate $M_d(E)\otimes M_b(E)=M_{db}(E)$.
117
+ Choose finitely many integral algebra elements whose reductions
118
+ form a matrix basis. Their determinant is a unit, so they remain
119
+ independent over $E((\varepsilon))$, proving full generation.
120
+
121
+ The representations defined by different $C_i$ have distinct kernels.
122
+ Indeed,
123
+ \[
124
+ \operatorname{tr}f_1(C_i)
125
+ =\varepsilon d\operatorname{tr}P_{i,1}^{\circ}
126
+ +O(\varepsilon^2),
127
+ \]
128
+ and the leading coefficients differ. Equal kernels would induce an
129
+ isomorphism of the full matrix images carrying every polynomial
130
+ evaluation in one to the other. Such an isomorphism preserves trace:
131
+ the trace of left multiplication is matrix size times matrix trace.
132
+ This contradicts the display.
133
+ The kernels are therefore distinct maximal two-sided ideals.
134
+ Evaluation is onto their finite product. Explicitly, for each pair
135
+ $i\ne j$ choose a polynomial vanishing in block $j$ and equal to
136
+ the identity in block $i$. The product over $j\ne i$ vanishes in
137
+ all other blocks and is the identity in block $i$; multiplying by
138
+ a lift of any matrix gives that product coordinate.
139
+
140
+ For the last assertion, compare the inner columns and arrow columns
141
+ at $P_i=P_j=0$. The inner image is
142
+ $J(X_0)\otimes M_b$, of dimension $(d^2-1)b^2$. The arrow derivative
143
+ is
144
+ \[
145
+ X_1\otimes U_1+X_2\otimes U_2.
146
+ \]
147
+ The original transverse independence implies that the combined map
148
+ has rank $(d^2+1)b^2$ at this reduction. Its generic rank is at
149
+ least this number. At a generic pair, the inner map has rank at
150
+ most $(db)^2=d^2b^2$; in fact it is injective, since a nonzero
151
+ intertwiner between the two simple representations would identify
152
+ their kernels. Subtracting this generic inner rank leaves at least
153
+ $b^2$ independent arrow directions in the quotient. A generic
154
+ fixed arrow consequently has nonzero quotient class.
155
+ \end{proof}
156
+
157
+ All determinant conditions in Lemma~\ref{lem:generic-generating-blocks}
158
+ hold on the same independent block and arrow coordinates used in
159
+ the division realization. Only finitely many blocks and arrows are
160
+ involved, so their nonzero minors can be imposed simultaneously.
161
+ In particular, the argument does not require replacing that realization
162
+ by a different choice of data.
163
+
164
+ We next isolate the translation argument. Its hypotheses concern
165
+ only the constant and linear coefficients; higher-order corrections
166
+ may be arbitrary.
167
+
168
+ \begin{lemma}[A translation preserving two directions]
169
+ \label{lem:translation-two-directions}
170
+ Let $E$ be a field of characteristic zero, let $n\ge1$ be an integer,
171
+ let $m=11$, and index
172
+ the blocks of $M_{mn}(E)$ by $\mathbb Z/m\mathbb Z$.
173
+ Suppose
174
+ \[
175
+ Y(s_1,s_2)\in M_{mn}(E)
176
+ \langle\!\langle s_1,s_2\rangle\!\rangle^u
177
+ \]
178
+ has constant tuple $C=\operatorname{diag}(C_i)$ generating
179
+ $\prod_iM_n(E)$. Suppose its two linear coefficients have the
180
+ following supports:
181
+ \[
182
+ (Y_1)_{ij}=0\ \text{unless }i-j\in\{1,2\},
183
+ \qquad
184
+ (Y_2)_{ij}=0\ \text{unless }i-j\in\{3,4\}.
185
+ \]
186
+ Assume every displayed edge coefficient is nonzero modulo the
187
+ cross-inner image $\{C_iT-TC_j:T\in M_n(E)\}$.
188
+ For a new central Laurent parameter $\gamma$, define
189
+ \[
190
+ Y'(s'_1,s'_2)=Y(\gamma+s'_1,s'_2).
191
+ \]
192
+ Then $Y'_0=Y(\gamma,0)$ generates $M_{mn}(E((\gamma)))$, and
193
+ $Y'_1,Y'_2$ are independent modulo $J(Y'_0)$.
194
+ \end{lemma}
195
+
196
+ \begin{proof}
197
+ The substitution is well-defined. In the coefficient of a fixed
198
+ new word, a contribution from an old word of length $r$ contains
199
+ $r$ minus the new word length factors of $\gamma$. Thus only
200
+ finitely many terms contribute at each $\gamma$ degree. Coefficients
201
+ converge in $E[[\gamma]]$, and the substitution respects products.
202
+
203
+ Let $B=\prod_iM_n(E)$ and let $I_C$ be the kernel of evaluation of
204
+ the free algebra at $C$. First-letter differentiation on $I_C$
205
+ has image a $B$-bimodule in $M_{mn}(E)$. Its projection onto every
206
+ first-color edge is nonzero. Otherwise the derivative into that
207
+ cross bimodule would descend to a derivation $\delta:B\to M_n(E)$,
208
+ where the left and right actions are through the distinct endpoint
209
+ factors $i,j$. Such a derivation is inner. In fact, for the central
210
+ idempotent $e_i$ of factor $i$, differentiating $e_i a=a e_i$ gives
211
+ \[
212
+ \delta(a)=a_iT-Ta_j,\qquad T=\delta(e_i).
213
+ \]
214
+ Applied to the generators, this contradicts the transverse edge
215
+ hypothesis. Since each full rectangular block is a simple bimodule
216
+ for its two matrix factors, the derivative image contains the full
217
+ block on every first-color edge.
218
+
219
+ Divide the corresponding evaluations of elements of $I_C$ at
220
+ $Y(\gamma,0)$ by $\gamma$. Their reductions supply all these edge
221
+ blocks. Ordinary evaluations already supply the full diagonal
222
+ product. The offset-one edges form a directed cycle through all
223
+ vertices, so products supply every matrix block. A finite set of
224
+ such elements with independent reductions therefore proves that
225
+ $Y(\gamma,0)$ generates the full matrix algebra.
226
+
227
+ It remains to check the two directions. Put $N=mn$ and
228
+ $J_0=J(C)$. Since $C$ generates $B$, its commutant consists of the
229
+ $m$ block scalars. Hence $\dim J_0=N^2-m$. Choose $N^2-m$ inner
230
+ columns with independent reductions spanning $J_0$. For a block
231
+ scalar $c=\operatorname{diag}(c_i I_n)$, the additional column
232
+ \[
233
+ \gamma^{-1}[c,Y(\gamma,0)]
234
+ \]
235
+ is integral and reduces to $[c,Y_1]$. These columns have rank
236
+ $m-1$ modulo $J_0$. Indeed, $[c,Y_1]\in J_0$ forces $c_i=c_j$
237
+ on each offset-one edge, by its transverse hypothesis, and the
238
+ cycle forces all $c_i$ to agree.
239
+
240
+ The two shifted linear coefficients reduce to $Y_1,Y_2$. Suppose
241
+ \[
242
+ aY_1+bY_2\in J_0+\{[c,Y_1]:c\text{ is block scalar}\}.
243
+ \]
244
+ At a second-color edge, only $bY_2$ contributes outside $J_0$,
245
+ so $b=0$. On the directed offset-one cycle, the relation then
246
+ forces $a=c_i-c_j$ on each edge. Summing gives $ma=0$, whence
247
+ $a=0$ in characteristic zero. Thus these two reductions are
248
+ independent modulo the enlarged inner-column space.
249
+
250
+ We have found $N^2-m+(m-1)+2=N^2+1$ independent reductions among
251
+ inner columns and the two tangents. They lift to independent
252
+ columns over $E((\gamma))$. Full generation of $Y'_0$ implies
253
+ $\dim J(Y'_0)=N^2-1$, so the two tangent classes are independent.
254
+ \end{proof}
255
+
256
+ Apply the lemma to $Y=X(Z)$. Lemma~\ref{lem:generic-generating-blocks}
257
+ supplies its diagonal-product and edge hypotheses, while the
258
+ eleven-block construction supplies precisely the two color supports.
259
+ Consequently the translated tuple generates after splitting and has
260
+ two independent tangent classes. These are finite rank conditions,
261
+ so they also hold over the division algebra's own center.
262
+ The central Laurent extension by $\gamma$ preserves division.
263
+ Both the old polynomial identities and the new algebraic relation
264
+ are preserved by the convergent substitution.
265
+
266
+ \subsection{Returning to a countable center}
267
+
268
+ The complete Laurent fields used so far need not be countable.
269
+ We finish by retaining only the scalar data required by the result.
270
+ Use the notation of Section~\ref{sec:division-realization}:
271
+ $F_0=H_0(a_*)$ is the construction field, $D_0$ is the central
272
+ division algebra over it, and
273
+ \[
274
+ L=F_0((\varepsilon))((\gamma))
275
+ \]
276
+ is the full shifted Laurent center. The field $F_0$ is countable:
277
+ $L_0$ is generated by finitely many indeterminates over the countable
278
+ field $k(\alpha,\beta)$, and $H_0$ is a subfield of $L_0$.
279
+ The algebra $D_0$ has degree $dbm$, and $D_0\otimes_{F_0}L$
280
+ is the central division algebra just constructed.
281
+
282
+ Choose an $F_0$-basis of $D_0$. Let $k'\subseteq L$ be the field
283
+ generated by $F_0$, the coefficients of the monic polynomial $q$
284
+ (taken to be $q_0$ when $q_0(w)=0$),
285
+ and every scalar coordinate in this basis of every coefficient
286
+ of the translated series $X'$ and $w'$. There are countably many
287
+ free words and finitely many coordinates per coefficient, so $k'$
288
+ is countable. Put
289
+ \[
290
+ A'=D_0\otimes_{F_0} k'.
291
+ \]
292
+ This is central simple of degree $dbm$. Its scalar extension to
293
+ $L$ is division, so $A'$ embeds in a division ring and has no zero
294
+ divisors. A finite-dimensional algebra without zero divisors is
295
+ a division algebra. Thus $A'/k'$ has the required central division
296
+ property and strictly larger degree.
297
+
298
+ All coefficients of $X',w'$ and $q$ lie in this smaller model.
299
+ The identities descend by its injective scalar extension to $L$.
300
+ Generation and transverse independence descend as well, since
301
+ the ranks of the finite coordinate matrices defining them do not
302
+ change under field extension. This proves every conclusion of
303
+ Theorem~\ref{thm:lifting}.
304
+
305
+ In the unconstrained case $q_0(w)=0$, the same argument applies
306
+ without the spectral corrections: use the same eleven-block
307
+ generic constant and colored linear terms, retain the relation
308
+ $q_0$, and carry out the translation and countable restriction
309
+ above. Thus that case also increases degree while preserving
310
+ generation and both directions.
preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/global-defect.tex ADDED
@@ -0,0 +1,298 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{The common space of spectral relations}
2
+ \label{sec:global-defect}
3
+
4
+ The active space describes the possible responses at one block. We now
5
+ identify the relations that remain when many independent blocks are used
6
+ together. The essential point is that the derivatives at different
7
+ triangular inputs belong to one common space. A bound on their ranks
8
+ separately would not give the relations needed for the free-series
9
+ construction.
10
+
11
+ We retain the preceding notation. The allowed sizes are
12
+ \(\mathcal S=\{pN:N\geq1\}\); at size \(n\in\mathcal S\), there are
13
+ \(e_n=dn/t\) distinct generic roots, each of multiplicity \(t\).
14
+ The active space has dimension \(a_n\), and \(\rho_n\) is the generic
15
+ rank of the eigenvalue differential, equivalently of the trace
16
+ differential. In particular \(\rho_n\leq a_n\).
17
+ We use the replication identity \(a_{pN}=Na_p\) and the following
18
+ consequence of the preceding attainability argument. There are a size
19
+ \(r\in\mathcal S\) and an integer \(K_0\geq1\) such that the loop
20
+ responses at a generic size-\(r\) point, together with paired responses
21
+ through \(K_0\) independent generic size-\(r\) partners, span its
22
+ active space. In each pairing, either arrow may be fixed generically
23
+ and the opposite arrow varied. All spaces below are extended to a
24
+ common splitting field when several independent points are involved.
25
+
26
+ \begin{lemma}[Derivatives at a star]
27
+ \label{lem:star-derivatives}
28
+ Let allowed-size blocks, evaluated by the preceding formal
29
+ specialization conventions, have split semisimple outputs with
30
+ disjoint spectra and the maximal total number of roots. Add input
31
+ arrows only from designated
32
+ hub blocks to designated leaf blocks, with no arrows between hubs or
33
+ between leaves. The resulting input has the same roots and
34
+ multiplicities as its diagonal part. A loop derivative at a block is
35
+ its loop response \(D\), with zero entries at all other blocks. If
36
+ \(U\) is a forward arrow between a leaf \(P\) and a hub \(Q\), a
37
+ derivative in its reverse arrow \(V\) has entries
38
+ \[
39
+ \bigl(m_h(P,Q;U,V)\bigr)_h,
40
+ \qquad
41
+ \bigl(m_k(Q,P;V,U)\bigr)_k
42
+ \]
43
+ at these two blocks and zero entries at the others.
44
+ \end{lemma}
45
+
46
+ \begin{proof}
47
+ Order the leaves before the hubs. The input and its evaluated output
48
+ are block upper triangular. The diagonal output blocks are the
49
+ original ones; since their spectra are disjoint, the output is similar
50
+ to their direct sum. In particular it is semisimple with the stated
51
+ roots and multiplicities.
52
+
53
+ Differentiate \(\operatorname{tr}(W^j)\). A closed block path
54
+ contributing to a reverse-arrow derivative must use that reverse
55
+ arrow once and its matching forward arrow once. There is no other
56
+ way to return to the starting block in this star. Its contribution
57
+ is therefore exactly the mixed-arrow contribution at the diagonal
58
+ input. Loop derivatives use no off-diagonal return. The previously
59
+ proved mixed-response formula gives the displayed pairs after
60
+ converting trace derivatives to root derivatives. This conversion is
61
+ invertible on all distinct roots: its entries are
62
+ \(jt\lambda_h^{j-1}\), and the corresponding Vandermonde determinant
63
+ is nonzero. The same reasoning applies to specialized blocks whenever
64
+ the stated maximal-count and disjointness hypotheses hold.
65
+ \end{proof}
66
+
67
+ \begin{lemma}[A stable upper bound for the differential rank]
68
+ \label{lem:tail-defect}
69
+ One can choose an arbitrarily large allowed size \(b\) and integers
70
+ \(a=a_b\) and \(g\geq0\), such that
71
+ \[
72
+ \rho_b=a-g,
73
+ \qquad
74
+ \rho_{bM}\leq Ma-g \quad(M\geq1).
75
+ \]
76
+ At a generic size-\(b\) point choose one root from each part of the
77
+ active partition. Projection onto these \(a\) selected roots
78
+ identifies the active space with the full coordinate space. The
79
+ quotient of that coordinate space by the loop-response image has
80
+ dimension \(g\).
81
+ \end{lemma}
82
+
83
+ \begin{proof}
84
+ For \(N\geq1\), put
85
+ \[
86
+ g_N=Na_r-\rho_{rN}.
87
+ \]
88
+ Replication and \(\rho_{rN}\leq a_{rN}\) show that \(g_N\geq0\).
89
+ For \(N\geq K_0\), take \(K_0\) of \(N\) independent size-\(r\)
90
+ blocks as hubs and the remainder as leaves. By
91
+ Lemma~\ref{lem:star-derivatives} and the attainability property, the
92
+ projection of the derivative image onto the leaf active spaces is
93
+ surjective. Reverse-arrow variables belonging to different leaves
94
+ are independent. Thus
95
+ \[
96
+ \rho_{rN}\geq(N-K_0)a_r,
97
+ \qquad g_N\leq K_0a_r.
98
+ \]
99
+ Here the specialized rank is bounded by the generic rank by the
100
+ formal minor identities. The finitely many smaller values of \(N\)
101
+ do not affect boundedness.
102
+
103
+ A bounded sequence of nonnegative integers has an eventual minimum
104
+ that is attained arbitrarily late. Choose \(N_0\geq K_0\) at such
105
+ an occurrence, and write
106
+ \[
107
+ g=g_{N_0},\qquad
108
+ g_N\geq g\ (N\geq N_0),\qquad
109
+ b=rN_0,\qquad a=N_0a_r.
110
+ \]
111
+ Then \(a=a_b\), \(\rho_b=a-g\), and
112
+ \[
113
+ \rho_{bM}=Ma-g_{N_0M}\leq Ma-g.
114
+ \]
115
+ No eventual constancy of \(g_N\) is required. Finally, the active
116
+ partition says that projection to one representative of each part
117
+ is an isomorphism on the active space. The loop image has rank
118
+ \(\rho_b\), so its quotient has dimension \(g\).
119
+ \end{proof}
120
+
121
+ Fix \(b,a,g\) as in Lemma~\ref{lem:tail-defect}. For each generic
122
+ size-\(b\) point \(P\), let \(E_P\) be the \(a\)-dimensional
123
+ space of selected-root coordinates, and let
124
+ \[
125
+ L_P=\operatorname{im}D_P\subseteq E_P,
126
+ \qquad H_P=E_P/L_P.
127
+ \]
128
+ Thus \(\dim H_P=g\). We regard \(H_P^*\) as the space of
129
+ covectors on \(E_P\) annihilating all loop responses.
130
+
131
+ \begin{lemma}[Surjectivity at both ends of a pair]
132
+ \label{lem:pair-quotient-surjectivity}
133
+ Let \(P,Q\) be independent generic size-\(b\) points. For a fixed
134
+ generic arrow \(U\) between them, varying the reverse arrow \(V\)
135
+ gives a joint paired-response map into \(H_P\oplus H_Q\) whose
136
+ projection to either summand is surjective. This holds whichever
137
+ orientation is fixed.
138
+ \end{lemma}
139
+
140
+ \begin{proof}
141
+ Specialize \(P\) and \(Q\) to diagonal sums of \(N_0\)
142
+ independent size-\(r\) points. For each little block in \(P\), the
143
+ \(N_0\geq K_0\) blocks in \(Q\), together with their components
144
+ of the fixed generic arrow, provide enough partners to span its
145
+ active space after loop columns are included. The reverse-arrow
146
+ entries touching different little blocks of \(P\) vary independently.
147
+ Compression at a root of one little block sees only the reverse
148
+ entries at that block. Consequently loops and paired columns span
149
+ all \(N_0a_r=a\) active coordinates at the \(P\)-end.
150
+
151
+ The resulting nonzero rank minor persists at generic \(P,Q,U\).
152
+ The labeled root data and the pair inverses are regular at the
153
+ disjoint diagonal specialization, so this is precisely the
154
+ determinant specialization justified earlier. Passing to the loop
155
+ quotient gives surjectivity onto \(H_P\). The same proof works at
156
+ the \(Q\)-end and with the other orientation fixed. The finitely
157
+ many nonzero minor conditions hold simultaneously on a nonempty
158
+ generic set.
159
+ \end{proof}
160
+
161
+ The next lemma supplies the common subspace promised at the start
162
+ of this section. Its formal-coordinate argument is the reason we
163
+ obtain compatible relations between pairs of blocks.
164
+
165
+ \begin{lemma}[A common tangent space]
166
+ \label{lem:common-tangent}
167
+ Fix \(M\geq1\) independent generic size-\(b\) points and their
168
+ selected roots. At inputs with this diagonal and arbitrary strictly
169
+ upper block arrows, the collective span of all selected-root
170
+ derivative columns has dimension at most \(Ma-g\). The span of
171
+ all loop columns and all two-block paired columns has dimension
172
+ exactly \(Ma-g\).
173
+ \end{lemma}
174
+
175
+ \begin{proof}
176
+ Put \(R=Ma-g\). For \(M=1\) the assertion is the definition of
177
+ the loop rank, so suppose \(M\geq2\). Use one block as a hub,
178
+ ordered last. The loops span \(\bigoplus_i L_{P_i}\), of dimension
179
+ \(M(a-g)\). Modulo that space, reverse derivatives project
180
+ surjectively onto each of the \(M-1\) leaf quotients by
181
+ Lemma~\ref{lem:pair-quotient-surjectivity}. These projections vary
182
+ independently. The derivative rank at this star is therefore at
183
+ least
184
+ \[
185
+ M(a-g)+(M-1)g=R.
186
+ \]
187
+ The generic upper bound in Lemma~\ref{lem:tail-defect} is \(R\).
188
+ Thus at a generic strictly upper-arrow array \(\mathcal U\) the
189
+ selected-root derivative rank equals \(R\).
190
+
191
+ Work over the field containing \(\mathcal U\) and the diagonal
192
+ splitting data. Let \(F(H)\) be the formal Taylor map of the
193
+ selected root shifts under unrestricted input-entry perturbations
194
+ \(H\). The base has the maximal root count, so the scalar branch
195
+ construction applies. Every \((R+1)\)-minor of \(dF\) is zero,
196
+ and some \(R\)-minor is a unit at \(H=0\). Choose the corresponding
197
+ \(R\) output coordinates and use them, together with the remaining
198
+ input coordinates, as new formal source coordinates \((y,z)\).
199
+ The formal inverse theorem gives
200
+ \[
201
+ F(y,z)=(y,G(y,z)).
202
+ \]
203
+ The vanishing \((R+1)\)-minors now imply
204
+ \(\partial G/\partial z=0\). In characteristic zero, coefficientwise
205
+ differentiation gives \(G(y,z)=G(y)\). At any formal source point
206
+ where \(F=0\), all derivative columns therefore belong to the fixed
207
+ graph
208
+ \[
209
+ \{(v,dG(0)v):v\in E^R\}.
210
+ \]
211
+
212
+ Shifting only the strictly upper arrows leaves every root unchanged.
213
+ Apply the preceding conclusion to these shifts: their Jacobian
214
+ columns all belong to this one graph, not merely to spaces of the
215
+ same dimension.
216
+
217
+ It remains to pass from formal shifts at \(\mathcal U\) to all
218
+ upper-arrow arrays. Let \(J(U)\) be the selected Jacobian at such
219
+ an array. It is polynomial in \(U\). Indeed a trace derivative
220
+ has just one differentiated input step, and every other
221
+ off-diagonal step is strictly upper; a contributing block path
222
+ therefore uses a bounded number of upper arrows. The remaining
223
+ diagonal sums converge by smallness. The conversion from trace
224
+ derivatives to root derivatives has coefficients depending only
225
+ on the fixed diagonal roots, so it preserves polynomial dependence.
226
+
227
+ Every covector annihilating the preceding graph annihilates the
228
+ polynomial matrix \(J(\mathcal U+S)\) as a formal identity in
229
+ the upper-arrow shift \(S\). Substitution \(S=V-\mathcal U\)
230
+ is valid in this polynomial identity. Hence it annihilates every
231
+ coefficient of \(J(V)\). The span of those coefficients, formed
232
+ over the original diagonal field, has dimension at most \(R\),
233
+ since scalar extension preserves rank. It contains every specialized
234
+ column and proves the collective-span assertion.
235
+
236
+ Loop columns occur at the diagonal input. A paired column supported
237
+ on two blocks occurs at the base with just the corresponding single
238
+ upper arrow, by Lemma~\ref{lem:star-derivatives}. Allowing both
239
+ arrows to vary makes the collection independent of which orientation
240
+ is called forward. All these columns therefore lie in the common
241
+ space. The one-hub star already gives \(R\) independent columns
242
+ among them, proving equality.
243
+ \end{proof}
244
+
245
+ \begin{proposition}[Compatible dual relations]
246
+ \label{prop:compatible-relations}
247
+ For any finite nonempty collection of independent generic size-\(b\)
248
+ points \(P_i\), there is a \(g\)-dimensional space
249
+ \[
250
+ \mathcal G_{\{P_i\}}\subseteq\bigoplus_i H_{P_i}^*
251
+ \]
252
+ with the following properties.
253
+ \begin{enumerate}
254
+ \item Projection to each \(H_{P_i}^*\) is an isomorphism.
255
+ \item It annihilates all joint paired responses, with both arrows
256
+ arbitrary.
257
+ \item For a fixed generic arrow between \(P_i,P_j\), the
258
+ annihilator in \(H_{P_i}^*\oplus H_{P_j}^*\) of the variable
259
+ reverse-arrow image is exactly the restriction of
260
+ \(\mathcal G_{\{P_i\}}\).
261
+ \item On adjoining independent blocks, restriction of the larger
262
+ space is the original space after scalar extension.
263
+ \end{enumerate}
264
+ For one block this space is \(H_P^*\). These statements include
265
+ \(g=0\).
266
+ \end{proposition}
267
+
268
+ \begin{proof}
269
+ Define \(\mathcal G\) as the annihilator of all loop and joint
270
+ paired columns in the selected coordinate space. By
271
+ Lemma~\ref{lem:common-tangent}, it has dimension \(g\); annihilation
272
+ of loops identifies it with a subspace of \(\bigoplus_i H_{P_i}^*\).
273
+ If an element has zero component at one vertex \(i\), its pairing
274
+ with columns on \((i,j)\) and the surjectivity onto \(H_{P_j}\)
275
+ force its component at every other vertex \(j\) to vanish.
276
+ Projection onto any one component is therefore injective, and hence
277
+ an isomorphism by dimension.
278
+
279
+ For a fixed generic arrow on \((i,j)\), the reverse-image in
280
+ \(H_{P_i}\oplus H_{P_j}\) has dimension at least \(g\), since
281
+ its projection onto either summand is surjective. It is killed by
282
+ the \(g\)-dimensional restriction of \(\mathcal G\). The latter's
283
+ annihilator has dimension \(2g-g=g\), so these two spaces coincide.
284
+ This proves the exact pairwise assertion.
285
+
286
+ Finally, restriction from a larger collection annihilates every old
287
+ loop and pair column. It is injective, because projection to any
288
+ retained vertex is injective, and both spaces have dimension \(g\).
289
+ It is therefore onto. For a single block the same statement follows
290
+ from its quotient dimension. All dimension arguments remain valid
291
+ when \(g=0\).
292
+ \end{proof}
293
+
294
+ We henceforth write \(\mathcal G\) for these compatible spaces,
295
+ specifying the blocks when needed. We have identified all linear
296
+ relations shared by the loop and paired corrections. The next
297
+ section proves that the leading free-word errors satisfy the
298
+ corresponding cyclic relations.
preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/introduction.tex ADDED
@@ -0,0 +1,139 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Introduction}\label{sec:introduction}
2
+
3
+ A division ring $D$ is \emph{algebraic over its center} $F=Z(D)$ if every
4
+ $a\in D$ satisfies a nonzero polynomial in $F[t]$. For a subset $S\subseteq D$,
5
+ write $F(S)$ for the division subring generated by $F\cup S$.
6
+ The ring is \emph{locally finite} if
7
+ \[
8
+ [F(S):F]<\infty\qquad\text{for every finite subset }S\subseteq D.
9
+ \]
10
+ The Kurosh problem for division rings asks whether algebraicity over the
11
+ center implies local finiteness. We give a negative answer.
12
+
13
+ All rings and subrings in this paper have the same identity. If $k$ is a
14
+ central subfield and $x,y$ belong to a ring, $k[x,y]$ denotes the unital
15
+ $k$-algebra generated by $x,y$; the generators need not commute.
16
+ The free polynomial algebra on two formal generators is denoted
17
+ $k\langle x,y\rangle$.
18
+
19
+ \begin{theorem}\label{thm:main}
20
+ There is a countable division ring $D$ of characteristic zero, with
21
+ center $F=Z(D)$, and elements $x,y\in D$ such that
22
+ \[
23
+ D=F[x,y]=F(x,y),\qquad [D:F]=\infty,
24
+ \]
25
+ while every element of $D$ is algebraic over $F$.
26
+ \end{theorem}
27
+
28
+ The same pair $\{x,y\}$ therefore witnesses the failure of local finiteness.
29
+ The construction does not prescribe the center. It first produces an
30
+ algebraic division ring over a countable central subfield, and a separate
31
+ finite-descent argument proves infinite dimension over the actual center.
32
+ The annihilating polynomial is allowed to depend on the element.
33
+
34
+ \subsection{Historical context}
35
+
36
+ Kurosh formulated his question in 1941 in connection with Burnside's
37
+ finiteness problem for groups. He asked whether a division ring that is
38
+ algebraic and finitely generated as an algebra over a central subfield
39
+ must be finite-dimensional over that subfield
40
+ \cite[Problem~(K), p.~240]{Kurosh1941}. The subfield in this formulation
41
+ need not be the full center, and finite generation means algebra
42
+ generation, not merely division generation.
43
+
44
+ The broader problem for algebraic algebras has a different history.
45
+ Golod's construction, based on the Golod--Shafarevich estimates, gives
46
+ finitely generated infinite-dimensional nil algebras
47
+ \cite[Example~1]{Golod1964}. Their unitizations are algebraic algebras
48
+ with nonzero nilpotents, so they do not answer the division-ring question.
49
+
50
+ There are positive results under additional hypotheses. Jacobson's
51
+ bounded-degree theorem gives a polynomial identity, and Kaplansky's
52
+ theorem makes algebraic algebras satisfying a polynomial identity
53
+ locally finite; see \cite[Theorems~3 and~5]{Jacobson1952}.
54
+ Bell, Drensky, and Sharifi later proved that a division ring whose
55
+ elements satisfy nonzero polynomial relations of uniformly bounded degree $d$,
56
+ with coefficients on the left in a possibly noncentral subfield, has
57
+ dimension at most $d^2$ over its center
58
+ \cite[Theorem~1.3]{BellDrenskySharifi2013}. Our construction imposes
59
+ element-dependent relations without a uniform degree bound.
60
+
61
+ Amitsur proved that a division algebra finitely generated as an algebra
62
+ over an uncountable central field is automatically algebraic
63
+ \cite[Corollary~$2'$]{Amitsur1956}. This conclusion is algebraicity,
64
+ not local finiteness. Countability plays a different role here: it
65
+ allows us to schedule all polynomial expressions in the construction.
66
+ Goodearl and Letzter's recent work \cite{GoodearlLetzter2026} treats
67
+ nonfinite generation as an algebra for classes of transcendental skew
68
+ fields and explicitly distinguishes that question from the algebraic
69
+ Kurosh problem. Theorem~\ref{thm:main} concerns algebraic division rings
70
+ and their actual centers.
71
+
72
+ The proof combines standard division-algebra constructions with matrix
73
+ and formal-series calculations. Symbol and cyclic algebras provide
74
+ division-ring models for the generic block data
75
+ \cite[Section~2.5]{GilleSzamuely2006}. Traces organize cyclic word
76
+ relations \cite[Section~4]{Procesi1976}, while inner derivations describe
77
+ infinitesimal conjugation \cite[Theorem~8]{Jacobson1937Derivations}.
78
+ The lifting argument supplies the additional response, compatibility,
79
+ and generation statements needed to preserve two independent deformation
80
+ directions while imposing successive algebraic relations.
81
+
82
+ \subsection{The construction}
83
+
84
+ The main ingredient is Theorem~\ref{thm:lifting}. Its input is a tuple of
85
+ formal series in two noncommuting variables over a finite-dimensional
86
+ central division algebra. The constant tuple generates the coefficient
87
+ algebra, and the two linear coefficients are independent modulo changes
88
+ coming from conjugation. The theorem makes any prescribed series
89
+ algebraic over a larger countable central field. At the same time it
90
+ increases the degree of the division algebra, preserves all previous
91
+ polynomial identities, and restores both generation and the two independent
92
+ directions. These last requirements allow the construction to continue.
93
+
94
+ For the prescribed series $w$, the immediate goal is to find a formal
95
+ substitution $Z=(Z_1,Z_2)$ for which $w(Z)$ satisfies the minimal
96
+ polynomial of the chosen constant output $w(Z(0))$. The input $Z(0)$
97
+ is a nonzero generic input, small with respect to an auxiliary valuation,
98
+ not the original zero input.
99
+ After splitting
100
+ the coefficient algebra into matrices, we take the constant input to be
101
+ a diagonal sum of independent generic matrix pairs. Varying a diagonal
102
+ block gives a first eigenvalue response; adding an arrow to another block
103
+ and an arrow back gives a paired response. Sections~\ref{sec:formal-generic}
104
+ and~\ref{sec:responses} establish the formal evaluation rules and show that
105
+ these responses partition the eigenvalue labels into linked groups.
106
+
107
+ A transfer theorem puts each first unsolved noncommutative word coefficient
108
+ in the same response space. It also turns proportional responses into
109
+ functional relations between eigenvalue branches
110
+ (Sections~\ref{sec:word-transfer} and~\ref{sec:linkage-replication}).
111
+ The relations within each block then separate from a fixed-dimensional
112
+ space of relations among blocks. To test the latter, we repeat each block
113
+ and attach auxiliary blocks, called hubs. Individual hubs distinguish
114
+ repeat positions; a common hub compares them. This matrix test proves
115
+ that every leading error satisfies the required cyclic sums of word
116
+ coefficients (Sections~\ref{sec:global-defect} and~\ref{sec:cyclic-obstructions}).
117
+
118
+ An eleven-block arrangement of two colors supplies corrections whose
119
+ only obstructions are those cyclic sums. We solve the equations one word
120
+ length at a time in Section~\ref{sec:free-correction}. A cyclic division
121
+ algebra realizes these matrix calculations over a division ring, and a
122
+ Taylor translation restores generation and the two independent directions
123
+ (Sections~\ref{sec:division-realization} and~\ref{sec:generation}).
124
+ The corrections are solutions of finite affine linear systems; this is
125
+ what permits their descent from a splitting field to the division
126
+ algebra's center. If $w$ already satisfies its constant term's minimal
127
+ polynomial, the spectral correction is unnecessary, but realization
128
+ and translation are still needed to increase degree and restore the
129
+ iteration hypotheses.
130
+
131
+ Section~\ref{sec:countable-construction} first explains how the lifting
132
+ theorem yields Theorem~\ref{thm:main}. The fields introduced during the
133
+ iteration are countable, so every polynomial expression can be scheduled.
134
+ A division-ring ultraproduct retains the resulting relations. Its
135
+ two-generated subalgebra is already a division ring, and finite word
136
+ sets prove that its dimension over the central coefficient field is
137
+ infinite. The actual-center argument concludes this deduction. The
138
+ remaining sections prove the lifting theorem and all its required
139
+ compatibilities.
preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/lifting.tex ADDED
@@ -0,0 +1,81 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{The lifting theorem}\label{sec:lifting}
2
+
3
+ The construction proceeds through finite-dimensional central division
4
+ algebras. At each step we impose an algebraic relation on one prescribed
5
+ element while preserving the freedom to enlarge the algebra at the next step.
6
+ Formal power series in two noncommuting variables record that freedom.
7
+
8
+ For a $k$-algebra $A$, write
9
+ \[
10
+ A\langle\!\langle z_1,z_2\rangle\!\rangle
11
+ \]
12
+ for the ring of formal series in words in $z_1,z_2$, with coefficients
13
+ in $A$ commuting with the variables. Multiplication concatenates words
14
+ and multiplies their coefficients in their original order. The ring is
15
+ complete for the filtration by word length. For a tuple
16
+ $X=(X^{(1)},\ldots,X^{(u)})$ of such series, let $X_0\in A^u$ be its
17
+ constant tuple and let $X_1,X_2\in A^u$ be its coefficients of the two
18
+ individual letters. Thus the subscripts $1,2$ denote letters, not degrees.
19
+ Set
20
+ \begin{equation}\label{eq:inner-tangent}
21
+ J_A(X_0)=\{([T,X_0^{(1)}],\ldots,[T,X_0^{(u)}]):T\in A\},
22
+ \qquad [T,a]=Ta-aT.
23
+ \end{equation}
24
+ The classes of $X_1,X_2$ modulo this subspace describe changes of the tuple
25
+ that cannot be obtained by infinitesimal conjugation.
26
+
27
+ \begin{theorem}[Algebraic lifting]\label{thm:lifting}
28
+ Let $k$ be a countable field of characteristic zero containing every root
29
+ of unity, and let $A$ be a finite-dimensional central division algebra
30
+ over $k$. Suppose
31
+ $X\in A\langle\!\langle z_1,z_2\rangle\!\rangle^u$ satisfies:
32
+ \begin{enumerate}[label=\textup{(\roman*)}]
33
+ \item $X_0$ generates $A$ as a $k$-algebra;
34
+ \item $X_1,X_2$ have linearly independent classes in $A^u/J_A(X_0)$.
35
+ \end{enumerate}
36
+ For every $w\in A\langle\!\langle z_1,z_2\rangle\!\rangle$, there exist
37
+ a countable field extension $k'/k$, a central division algebra $A'/k'$ of
38
+ strictly larger degree, and series
39
+ \[
40
+ X'\in A'\langle\!\langle s_1,s_2\rangle\!\rangle^u,
41
+ \qquad w'\in A'\langle\!\langle s_1,s_2\rangle\!\rangle
42
+ \]
43
+ with the following properties:
44
+ \begin{enumerate}[label=\textup{(\alph*)}]
45
+ \item Every noncommutative polynomial identity over $k$ satisfied by the
46
+ tuple $(X,w)$ is satisfied by $(X',w')$ as an identity of formal series.
47
+ \item The constant tuple $X'_0$ generates $A'$ over $k'$, and the classes
48
+ of $X'_1,X'_2$ in $(A')^u/J_{A'}(X'_0)$ are linearly independent.
49
+ \item There is a monic nonzero polynomial $q\in k'[t]$ such that $q(w')=0$.
50
+ \end{enumerate}
51
+ Here the degree of a central division algebra $B/F$ is $\sqrt{[B:F]}$.
52
+ \end{theorem}
53
+
54
+ Theorem~\ref{thm:lifting} is the central construction. Its application to
55
+ the Kurosh problem uses $u=2$ and addresses one polynomial in the two
56
+ generators at a time. The fields are allowed to grow; they need not be
57
+ algebraic extensions of their predecessors. The final step will therefore
58
+ identify the actual center separately and prove infinite dimension over it.
59
+
60
+ Figure~\ref{fig:response-interfaces} separates the two tasks within a
61
+ lifting step. The response calculation makes the prescribed series
62
+ algebraic; the final translation restores the hypotheses needed to repeat
63
+ the step. The two transverse directions must survive together, not merely
64
+ one at a time.
65
+
66
+ \begin{figure}[tbp]
67
+ \centering
68
+ \input{figures/response-interfaces}
69
+ \caption{The spectral case of Theorem~\ref{thm:lifting}.
70
+ The two displayed classes at each end are linearly independent in the
71
+ indicated quotient. The middle boxes describe the matrix calculation:
72
+ allowable eigenvalue changes control the first unsolved word errors,
73
+ and the cyclic relations are precisely the obstructions to correction.
74
+ Realization and translation return a generating tuple over a division
75
+ algebra of strictly larger degree. If $w$ already satisfies the minimal
76
+ polynomial of $w(0)$, the middle spectral correction is omitted, but
77
+ realization and translation remain necessary. No embedding tower of
78
+ the successive division algebras is asserted.}
79
+ \label{fig:response-interfaces}
80
+ \end{figure}
81
+ \clearpage
preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/linkage.tex ADDED
@@ -0,0 +1,317 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Functional linkage and replication}
2
+ \label{sec:linkage-replication}
3
+
4
+ We now show that the dimension of the active response space is additive
5
+ under generic direct sums. The main point is to turn the linear relations
6
+ between linked responses into identities between eigenvalue branches.
7
+ These identities will continue to control responses through partners of
8
+ every allowed size.
9
+
10
+ Retain the progression $\mathcal S=\{pN:N\geq 1\}$ and the common
11
+ eigenvalue multiplicity $t$. Thus, at size $n\in\mathcal S$, the number
12
+ of distinct generic eigenvalues is $e_n=dn/t$. We use the following
13
+ previously established facts. At a direct sum of independent small
14
+ generic inputs of sizes in $\mathcal S$, the spectra are disjoint and
15
+ have the maximal number of distinct eigenvalues. Their commuting
16
+ Taylor deformations therefore have scalar spectral blocks, by
17
+ Lemma~\ref{lem:scalar-branches}. The response identities admit the
18
+ specializations of Lemma~\ref{lem:active-specialization}, and their
19
+ leading terms satisfy Proposition~\ref{prop:word-transfer}.
20
+
21
+ For a generic input $P$, let $\Omega_P$ be its spectral splitting
22
+ field, and choose a constant input direction $v$ such that
23
+ $D_h(P;v)\neq 0$ for every eigenvalue label $h$. Recall the active-space
24
+ partition $\mathcal P_P$, characterized by
25
+ \begin{equation}
26
+ \mathcal T_P
27
+ =\left\{c\in\Omega_P^{e_n}:
28
+ \frac{c_h}{D_h(P;v)}
29
+ \text{ is constant on each member of }\mathcal P_P\right\}.
30
+ \label{eq:linkage-partition}
31
+ \end{equation}
32
+ Labels in one member of this partition are called linked. In particular,
33
+ $a_n=\dim_{\Omega_P}\mathcal T_P$ is the number of its members.
34
+ The argument below uses the full coefficientwise definition of
35
+ $\mathcal T_P$: it contains the loop responses $D(P;Y)$ and the
36
+ coefficient vectors of $m(P,Q;U,V)$ for every partner size in
37
+ $\mathcal S$.
38
+
39
+ \subsection{A formal identity for linked branches}
40
+
41
+ \begin{proposition}[Functional linkage]
42
+ \label{prop:functional-linkage}
43
+ Let $P$ be a small generic input of size $p$, and let $h,h'$ be linked
44
+ labels at $P$. Let $C_1,\ldots,C_s$ be small generic inputs of sizes in
45
+ $\mathcal S$, jointly independent with $P$, where $s=0$ is allowed.
46
+ Put $R=\operatorname{diag}(P,C_1,\ldots,C_s)$.
47
+ Over a common spectral splitting field $E$, denote by
48
+ $\Lambda_j^R(\Delta)$ the scalar eigenvalue branch of $W(R+\Delta)$
49
+ whose value at zero is $\lambda_j(P)$, for $j=h,h'$.
50
+
51
+ Define
52
+ \[
53
+ g_j(\eta)=\lambda_j(P+\eta v)-\lambda_j(P)
54
+ \in\Omega_P[[\eta]],\qquad j=h,h'.
55
+ \]
56
+ Then $g_{h'}'(0)\neq 0$, and
57
+ \begin{equation}
58
+ \Lambda_h^R(\Delta)-\lambda_h(P)
59
+ =\bigl(g_h\circ g_{h'}^{-1}\bigr)
60
+ \bigl(\Lambda_{h'}^R(\Delta)-\lambda_{h'}(P)\bigr).
61
+ \label{eq:functional-linkage}
62
+ \end{equation}
63
+ Here $g_{h'}^{-1}$ denotes the inverse for composition. In particular,
64
+ the univariate series in this identity depends only on $P,h,h'$ and $v$,
65
+ and is unchanged when auxiliary blocks are adjoined.
66
+ \end{proposition}
67
+
68
+ \begin{proof}
69
+ We first explain why the response relations persist while $P$ moves.
70
+ By the Taylor convention in Section~\ref{subsec:formal-conventions},
71
+ substitution $P\mapsto P+\eta v$ gives homomorphisms
72
+ \[
73
+ \operatorname{Frac}K[[P]]
74
+ \longrightarrow \bigl(\operatorname{Frac}K[[P]]\bigr)[[\eta]],
75
+ \qquad
76
+ \Omega_P\longrightarrow\Omega_P[[\eta]],
77
+ \]
78
+ both reducing to the identity at $\eta=0$. The second uniquely
79
+ extends the first through the finite separable extension
80
+ $\Omega_P/\operatorname{Frac}K[[P]]$. Thus every nonzero element
81
+ has image with invertible constant term, and the eigenvalues and
82
+ projections map to their uniquely labeled Taylor deformations.
83
+
84
+ For linked labels, Equation~\eqref{eq:linkage-partition} gives
85
+ \begin{equation}
86
+ D_{h'}(P;v)c_h-D_h(P;v)c_{h'}=0
87
+ \label{eq:linked-response-relation}
88
+ \end{equation}
89
+ for every loop response and every coefficient vector of every paired
90
+ response. Apply the preceding homomorphism coefficientwise in the
91
+ partner coordinates. The resulting identities are exactly
92
+ Equation~\eqref{eq:linked-response-relation} at the moved input
93
+ $P+\eta v$, with the moved eigenvalues, projections, and $D$-factors.
94
+ They remain valid in the triangular specializations used in
95
+ Proposition~\ref{prop:word-transfer}. More explicitly, first clear the
96
+ finitely many auxiliary resolvent determinants. At each Taylor degree,
97
+ the number of strictly upper steps is bounded. This permits their
98
+ entries to have Laurent coefficients in $\eta$, while the diagonal
99
+ entries are expanded at the original small inputs. Coefficientwise
100
+ convergence and specialization are then supplied by
101
+ Lemma~\ref{lem:active-specialization}. Thus the transfer argument
102
+ applies over $E((\eta))$ with the transported response relation.
103
+
104
+ Write $v_R$ for $v$ supported in the $P$-block and put
105
+ $R(\eta)=R+\eta v_R$. At $R(\eta)+H$, impose the equation
106
+ \begin{equation}
107
+ \Lambda_{h'}^{R(\eta)}(H)=\lambda_{h'}(P+\eta v).
108
+ \label{eq:fixed-linked-branch}
109
+ \end{equation}
110
+ Choose linear coordinates $H=u v_R+H_{\mathrm{rest}}$, with
111
+ $H_{\mathrm{rest}}$ in a fixed complementary space of input directions.
112
+ The derivative of the left side in $u$ at $H=0$ is
113
+ $D_{h'}(P+\eta v;v)$, a unit in $E[[\eta]]$. Formal implicit
114
+ substitution therefore eliminates $u$. In particular, the quotient
115
+ of $E[[\eta,H]]$ by Equation~\eqref{eq:fixed-linked-branch} is
116
+ \begin{equation}
117
+ E[[\eta,H_{\mathrm{rest}}]],
118
+ \qquad
119
+ E[[\eta,H_{\mathrm{rest}}]]
120
+ \lhook\joinrel\longrightarrow
121
+ E((\eta))[[H_{\mathrm{rest}}]].
122
+ \label{eq:linkage-quotient-injection}
123
+ \end{equation}
124
+ The eliminated series has zero constant term in $H_{\mathrm{rest}}$.
125
+
126
+ On this quotient, scalar-block separation implies that the fixed-root
127
+ Schur expression $S_{h'}$ at $R(\eta)$ vanishes. We claim that $S_h$
128
+ also vanishes over the right-hand ring in
129
+ Equation~\eqref{eq:linkage-quotient-injection}. Induct on total degree
130
+ in $H_{\mathrm{rest}}$. Both Schur expressions vanish in degree zero.
131
+ If they vanish below degree $l$, the commuting-parameter conclusion of
132
+ Proposition~\ref{prop:word-transfer}, together with the transported
133
+ relation~\eqref{eq:linked-response-relation}, gives scalar leading
134
+ coefficients $[S_j]_l=c_{j,l}\pi_j$ for $j=h,h'$, with
135
+ \[
136
+ D_{h'}(P+\eta v;v)c_{h,l}
137
+ =D_h(P+\eta v;v)c_{h',l}=0.
138
+ \]
139
+ Here the $c_{j,l}$ are scalar homogeneous polynomials in the remaining
140
+ parameters over $E((\eta))$; the projections are the moved target
141
+ projections. The first factor is nonzero, so $c_{h,l}=0$ and
142
+ $[S_h]_l=0$.
143
+
144
+ It follows that the $h$-branch is fixed as well:
145
+ \[
146
+ \Lambda_h^{R(\eta)}(H)=\lambda_h(P+\eta v)
147
+ \]
148
+ on the quotient. For clarity, the implication from $S_h=0$ uses the
149
+ scalar blocks of Lemma~\ref{lem:scalar-branches}: the complementary
150
+ block at the fixed root is invertible, and the determinant of the full
151
+ matrix at that root is a unit times the $t$-th power of the shift of
152
+ the $h$-branch. The quotient is a domain, so the shift is zero.
153
+ Both branch series and the eliminated coordinate are regular in
154
+ $\eta$. The injection in
155
+ Equation~\eqref{eq:linkage-quotient-injection} therefore descends this
156
+ equality to $E[[\eta,H_{\mathrm{rest}}]]$.
157
+
158
+ Finally make the invertible linear coordinate change
159
+ $\Delta=H+\eta v_R$. Equation~\eqref{eq:fixed-linked-branch} becomes
160
+ \[
161
+ \Lambda_{h'}^R(\Delta)-\lambda_{h'}(P)=g_{h'}(\eta).
162
+ \]
163
+ Since $g_{h'}'(0)=D_{h'}(P;v)\neq0$, it eliminates $\eta$ as
164
+ $g_{h'}^{-1}(\Lambda_{h'}^R(\Delta)-\lambda_{h'}(P))$.
165
+ Substitution in the equality for the $h$-branch gives
166
+ Equation~\eqref{eq:functional-linkage}.
167
+ \end{proof}
168
+
169
+ \subsection{All partner sizes and the dimension formula}
170
+
171
+ We next pass from an identity near a direct sum to an identity for
172
+ every coefficient defining the generic active space. This step is
173
+ necessary because a bound proved using a fixed collection of partners
174
+ would not bound $a_n$.
175
+
176
+ \begin{proposition}[Replication of active dimensions]
177
+ \label{prop:active-replication}
178
+ For every positive integer $N$,
179
+ \[
180
+ a_{pN}=N a_p.
181
+ \]
182
+ \end{proposition}
183
+
184
+ \begin{proof}
185
+ Put $n=pN$ and choose independent small generic inputs
186
+ $P_1,\ldots,P_N$ of size $p$. Write
187
+ $R_1=\operatorname{diag}(P_1,\ldots,P_N)$ and use
188
+ $x=R_1+\Delta_1$ to label the generic size-$n$ spectrum by its branches
189
+ at $R_1$.
190
+
191
+ This substitution embeds $K[[x]]$ in $E[[\Delta_1]]$. Indeed, for
192
+ an image of a series over $K$, the Taylor coefficients are uniformly
193
+ integral in the small parameter $\varepsilon$. Substituting
194
+ $\Delta_1=\varepsilon X-R_1$, with independent coordinates $X$,
195
+ is therefore convergent and recovers the original series at
196
+ $\varepsilon X$. Homogeneous expansion at that point detects every
197
+ nonzero series. The embedding extends to the fraction field. All
198
+ generic spectral roots are supplied by the scalar branches at $R_1$,
199
+ so it also embeds a spectral splitting field $\Omega_x$ into
200
+ $\operatorname{Frac}E[[\Delta_1]]$, with these labels. The branches
201
+ and spectral projections themselves are regular at $\Delta_1=0$.
202
+
203
+ Fix a block $i$ and labels $h,h'$ in one member of
204
+ $\mathcal P_{P_i}$. Choose a constant direction $v_i$ supported in
205
+ that block, nonzero under every $D_h(P_i;\cdot)$. Apply
206
+ Proposition~\ref{prop:functional-linkage} first at $R_1$.
207
+ Differentiating its identity gives proportional loop responses at
208
+ $x$. Now adjoin an independent generic partner $Q$ of any fixed
209
+ size in $\mathcal S$, and apply the same proposition to
210
+ $\operatorname{diag}(R_1,Q)$. Its univariate series is the same
211
+ one. At $\operatorname{diag}(x,Q)$, perturb the opposite input
212
+ blocks by $uU$ and $zV$. Either arrow alone preserves the spectrum,
213
+ so the first derivatives in $u$ and $z$ vanish. The coefficient of
214
+ $uz$ in the branch is the paired response $m_h(x,Q;U,V)$.
215
+ The mixed chain rule and the separate first derivative in $v_i$
216
+ give
217
+ \begin{equation}
218
+ D_{h'}(x;v_i)m_h(x,Q;U,V)
219
+ -D_h(x;v_i)m_{h'}(x,Q;U,V)=0.
220
+ \label{eq:replicated-pair-relation}
221
+ \end{equation}
222
+ The two $D$-factors have nonzero reductions at $\Delta_1=0$.
223
+
224
+ We must verify this relation coefficientwise in $Q$, rather than only
225
+ at its generic value. Cross multiplication has already removed the
226
+ response ratio. Multiply further by the finitely many determinants
227
+ of $W(Q)-\lambda_h(x)$ and $W(Q)-\lambda_{h'}(x)$ needed to clear
228
+ the auxiliary inverses. At each fixed $\Delta_1$-degree, the resulting
229
+ series in the independent coordinates of $Q$ has coefficients
230
+ uniformly bounded below in $\varepsilon$-valuation. The branch and
231
+ projection coefficients do not involve $Q$; the other factors are
232
+ ordinary matrix series with two prescribed arrow steps and a fixed
233
+ number of Taylor insertions. Their path expansions give precisely
234
+ this bound, as in Lemma~\ref{lem:admissible-evaluation}.
235
+ Evaluation at small generic $Q$ therefore detects every coefficient.
236
+ Equation~\eqref{eq:replicated-pair-relation} is consequently a
237
+ formal identity in those coordinates. Injectivity of the embedding
238
+ of $\Omega_x$ descends it to the generic size-$n$ field. Finally,
239
+ the cleared determinants have nonzero constant terms in $Q$, so
240
+ they can be canceled in $\Omega_x[[Q]]$.
241
+
242
+ This argument applies separately to every partner size with the same
243
+ labeling of $x$ and the same $D$-factors. It therefore gives a
244
+ relation on every coefficient vector used to define $\mathcal T_x$.
245
+ Together with the corresponding loop relations, it says that
246
+ $c_h/D_h(x;v_i)$ is constant on each old partition member within
247
+ block $i$, for every $c\in\mathcal T_x$. These partitions have
248
+ $Na_p$ members in total, and all their normalizing factors are
249
+ nonzero. Thus $a_n\leq Na_p$.
250
+
251
+ For the opposite inequality, use
252
+ Lemma~\ref{lem:active-specialization} for each $P_i$, choosing all
253
+ partners jointly independent. At $R_1$, support each loop direction,
254
+ and both arrows of each paired response, in its chosen block $i$.
255
+ The responses then coincide with the original responses on that
256
+ block and vanish on every other block. They have rank $Na_p$.
257
+ Evaluate the same finite collection first at $R_1+\Delta_1$.
258
+ All branch data and partner resolvents are regular at
259
+ $\Delta_1=0$, since the partner spectra are disjoint from that of
260
+ $R_1$. A generic rank bound smaller than $Na_p$ would make every
261
+ minor of that order vanish over the embedded generic field, and hence
262
+ also at the reduction. The displayed specialization contradicts this.
263
+ Therefore $a_n\geq Na_p$.
264
+ \end{proof}
265
+
266
+ \subsection{Partners of one common size}
267
+
268
+ The dimension formula permits us to use a fixed matrix size on both
269
+ ends of every paired response. We will also need to fix one arrow
270
+ and vary only its reverse.
271
+
272
+ \begin{corollary}[Equal-size partners]
273
+ \label{cor:equal-size-partners}
274
+ There are $r\in\mathcal S$ and a positive integer $K_0$ with the
275
+ following property. Let $P,Q_1,\ldots,Q_{K_0}$ be independent small
276
+ generic inputs of size $r$. For generic fixed input arrows
277
+ $U_j:P\leftarrow Q_j$, the loop columns and the images of
278
+ \[
279
+ V\longmapsto m(P,Q_j;U_j,V),
280
+ \qquad V:Q_j\leftarrow P,\quad 1\leq j\leq K_0,
281
+ \]
282
+ span $\mathcal T_P$ after extension to the joint field of the data.
283
+ The analogous assertion holds with the other arrow fixed. The same
284
+ $r$ and $K_0$ may be used for both assertions.
285
+ \end{corollary}
286
+
287
+ \begin{proof}
288
+ Choose a finite witness list at size $p$ from
289
+ Lemma~\ref{lem:active-specialization}, and let its partner sizes be
290
+ $q_1,\ldots,q_M\in\mathcal S$. Choose $r=pN$ with
291
+ $r\geq q_j$ for every $j$. Specialize the size-$r$ base to a direct
292
+ sum of $N$ independent size-$p$ inputs. For each block, use a fresh
293
+ copy of the witness list. Pad a size-$q_j$ partner to size $r$ by
294
+ adjoining independent generic diagonal data of size $r-q_j$, omitting
295
+ the padding if this difference is zero. Give both arrows zero entries
296
+ on the padding. The response remains the original size-$p$ witness
297
+ on its chosen base block and is zero on the other base blocks.
298
+
299
+ The resulting columns have rank $Na_p=a_r$ by
300
+ Proposition~\ref{prop:active-replication}. All inputs at this
301
+ specialization have maximal spectral count, and the partner spectra
302
+ are disjoint from the base spectrum. The regular-minor argument in
303
+ the preceding proof therefore transfers this rank to generic
304
+ size-$r$ base and partner inputs.
305
+
306
+ Assign a separate partner to every paired column in this finite
307
+ list. At the witness specialization, choose its forward arrow to
308
+ be the specified $U_j$ and test the variable reverse arrow on the
309
+ specified $V_j$. A minor of order $a_r$ is nonzero there. Since
310
+ paired responses are bilinear in their arrows, this minor remains
311
+ nonzero for generic fixed forward arrows and suitable reverse-arrow
312
+ columns. This proves the first assertion with finitely many partners.
313
+ The identical argument fixes the reverse arrows instead. Increasing
314
+ the number of independent partners to the larger of the two finite
315
+ numbers proves both assertions with one $K_0$. If no paired column
316
+ is needed, one unused generic partner may be added so that $K_0>0$.
317
+ \end{proof}
preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/responses.tex ADDED
@@ -0,0 +1,312 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{The space of eigenvalue responses}\label{sec:responses}
2
+
3
+ Fix a size $n\in\mathcal S$, a generic input pair $P$, and a splitting
4
+ field $\Omega_P$ of $W(P)$ over $\operatorname{Frac}K[[P]]$.
5
+ Write its distinct roots as $\lambda_h$, with spectral projections
6
+ $\pi_h$, $1\le h\le e_n$. Each projection has rank $t$.
7
+ We also use these data after embedding into the valued fields of
8
+ Section~\ref{sec:formal-generic}.
9
+
10
+ We seek the possible leading changes of the eigenvalues at $P$.
11
+ Besides varying $P$ itself, we allow an excursion through another
12
+ input block and a return to $P$. Their linear span will determine
13
+ which eigenvalues can be varied independently.
14
+
15
+ \subsection{Loop and paired responses}\label{subsec:response-formulas}
16
+
17
+ Upper triangular block evaluations are also the basic mechanism of
18
+ noncommutative difference-differential calculus; see
19
+ \cite[Proposition~2.2 and Theorem~3.11]{KaliuzhnyiVerbovetskyiVinnikov2014}.
20
+ Here the admissible evaluations of Section~\ref{sec:formal-generic}
21
+ let us extract scalar eigenvalue responses from those block calculations.
22
+
23
+ For a perturbation $\mathcal W$ of $W(P)$, put $\pi=\pi_h$,
24
+ $\bar\pi=1-\pi$, and
25
+ \[
26
+ C_h(\mathcal W)=\bar\pi(\mathcal W-\lambda_h)\bar\pi.
27
+ \]
28
+ This operator acts on the complementary space. Its constant term is
29
+ invertible, so its inverse has a unique expansion in either commuting
30
+ or free formal parameters. Define the fixed-root Schur expression by
31
+ \begin{equation}
32
+ S_h(\mathcal W)=
33
+ \pi(\mathcal W-\lambda_h)\pi
34
+ -\pi\mathcal W\bar\pi
35
+ C_h(\mathcal W)^{-1}
36
+ \bar\pi\mathcal W\pi.
37
+ \label{eq:fixed-schur}
38
+ \end{equation}
39
+ This expression records the obstruction to keeping the root $\lambda_h$
40
+ fixed. For $u$ in the image of $\pi$, the vector
41
+ \[
42
+ u-C_h(\mathcal W)^{-1}\bar\pi\mathcal W\pi u
43
+ \]
44
+ is the unique vector projecting to $u$ whose complementary component
45
+ under $\mathcal W-\lambda_h$ vanishes. Its remaining component is
46
+ $S_h(\mathcal W)u$. Thus $S_h(\mathcal W)=0$ means that the fixed-root
47
+ kernel is a graph over the original eigenspace.
48
+
49
+ When the constant output is split semisimple and these equations are
50
+ imposed for every one of its distinct roots, the kernel graphs combine
51
+ into a formal change of basis. The output remains conjugate to its
52
+ constant term and satisfies that constant term's minimal polynomial.
53
+ Lemma~\ref{lem:schur-polynomial} proves the equivalence with the
54
+ polynomial identity at every finite word order.
55
+
56
+ The same Schur expression is defined near $\operatorname{diag}(P,C_0)$
57
+ if $\lambda_h$ is absent from $W(C_0)$, embedding $\pi_h$ at the $P$
58
+ block. In this use, equations indexed by labels at $P$ record those
59
+ fixed roots only.
60
+
61
+ For a loop direction $Y=(Y_1,Y_2)$ at $P$, define the scalar
62
+ $D_h(P;Y)$ by
63
+ \begin{equation}
64
+ \pi_h W'_P(Y)\pi_h=D_h(P;Y)\pi_h.
65
+ \label{eq:loop-response}
66
+ \end{equation}
67
+ This compression is scalar: apply Lemma~\ref{lem:scalar-branches}
68
+ to the commuting deformation $P+xY$ and take its first coefficient.
69
+ Equivalently, $D_h(P;Y)$ is the differential of the branch
70
+ $\lambda_h$ in direction $Y$. By
71
+ Lemma~\ref{lem:nonconstant-roots}, each of these linear functionals is
72
+ nonzero. Because $K$ is infinite, we can choose a constant direction
73
+ $v$ over $K$ with
74
+ \begin{equation}
75
+ D_h(P;v)\ne0\qquad(1\le h\le e_n).
76
+ \label{eq:nonzero-direction}
77
+ \end{equation}
78
+ Indeed the forbidden directions form a finite union of proper
79
+ $K$-linear subspaces, even though their defining coefficients belong
80
+ to $\Omega_P$.
81
+
82
+ Let $Q$ be an independent generic point of size $n'\in\mathcal S$.
83
+ Let $U$ be an input arrow $P\leftarrow Q$ and $V$ an input arrow
84
+ $Q\leftarrow P$; each is a pair of rectangular scalar matrices.
85
+ Form the triangular input pair
86
+ \[
87
+ T=\begin{pmatrix}P&U&0\\0&Q&V\\0&0&P\end{pmatrix}.
88
+ \]
89
+ Set
90
+ \begin{equation}
91
+ M_h(P,Q;U,V)=\pi_h\left(
92
+ W(T)_{13}
93
+ -W(T)_{12}(W(Q)-\lambda_h)^{-1}W(T)_{23}
94
+ \right)\pi_h.
95
+ \label{eq:paired-response}
96
+ \end{equation}
97
+ Block paths show that this is bilinear in $U,V$. The inverse exists
98
+ because the spectra at independent points are disjoint.
99
+
100
+ \begin{lemma}\label{lem:paired-scalar}
101
+ There is a scalar $m_h(P,Q;U,V)$ such that
102
+ \[
103
+ M_h(P,Q;U,V)=m_h(P,Q;U,V)\pi_h.
104
+ \]
105
+ It is the coefficient of $xy$ in the branch reducing to $\lambda_h$
106
+ for the commuting input deformation
107
+ \[
108
+ \begin{pmatrix}P&xU\\yV&Q\end{pmatrix}.
109
+ \]
110
+ The same assertion holds at an admissible specialized pair whose
111
+ spectra are disjoint and whose combined output is split semisimple
112
+ with the maximal number $e_{n+n'}$ of distinct roots.
113
+ \end{lemma}
114
+
115
+ \begin{proof}
116
+ At $x=y=0$, disjointness and Lemma~\ref{lem:stable-multiplicity}
117
+ give $e_n+e_{n'}=e_{n+n'}$ roots. Thus
118
+ Lemma~\ref{lem:scalar-branches} applies. Either arrow alone leaves
119
+ the spectrum unchanged, so the chosen branch has no terms depending
120
+ on $x$ alone or on $y$ alone.
121
+
122
+ Compute the $xy$ coefficient of its fixed-root Schur expression.
123
+ The direct return from $P$ through $Q$ gives $W(T)_{13}$. Eliminating
124
+ the $Q$ block gives the second term in
125
+ \eqref{eq:paired-response}. The other eigenspaces in the $P$ block
126
+ give no further term of this order: their couplings to $\pi_h$ have
127
+ zero constant term and no first-order term under these off-diagonal
128
+ input perturbations. Replacing the fixed root by the scalar branch
129
+ subtracts its $xy$ coefficient times $\pi_h$. The resulting Schur
130
+ expression vanishes, because the branch eigenspace projects
131
+ isomorphically to the base eigenspace. This proves the formula.
132
+ The specialized assertion uses exactly the same argument and the
133
+ specialization-stable degree bound.
134
+ \end{proof}
135
+
136
+ \subsection{Coefficient spans and their specializations}
137
+ \label{subsec:active-space}
138
+
139
+ At $Q=0$ the matrices $W(Q)-\lambda_h$ are invertible, since no
140
+ $\lambda_h$ belongs to the spectrum of $w(0)$. Hence
141
+ \eqref{eq:paired-response} has a formal expansion in the entries of
142
+ $Q$ over $\Omega_P$. Define
143
+ \[
144
+ m_h=\frac1t\operatorname{tr}M_h,
145
+ \qquad m=(m_h)_{h=1}^{e_n},\qquad D=(D_h)_{h=1}^{e_n}.
146
+ \]
147
+ Here $D=D(P;\cdot):M_n(\Omega_P)^2\to\Omega_P^{e_n}$ is the linear
148
+ map of loop responses. Its columns are its values on the standard
149
+ coordinate directions in the two input matrices.
150
+ The scalar identity of Lemma~\ref{lem:paired-scalar} holds also for
151
+ these formal expansions, by clearing their determinants and applying
152
+ Lemma~\ref{lem:generic-detection}.
153
+
154
+ Define $\mathcal T_P\subseteq\Omega_P^{e_n}$ to be the linear span
155
+ of the columns of $D$ and of every coefficient vector of $m$, for
156
+ every allowed partner size $n'\in\mathcal S$ and every pair of
157
+ coordinate arrows $U,V$. Write
158
+ \[
159
+ a_n=\dim_{\Omega_P}\mathcal T_P.
160
+ \]
161
+ Although the definition permits infinitely many partner sizes and
162
+ coefficients, the ambient space is finite dimensional.
163
+
164
+ \begin{lemma}[Specialization and finite witnesses]
165
+ \label{lem:active-specialization}
166
+ The scalar identities for $M_h$ and every linear identity expressing
167
+ $m\in\mathcal T_P$ hold after any admissible specialization of the
168
+ partner input for which the required inverses exist. For identities
169
+ on a subset of labels, only the inverses for those labels are needed.
170
+
171
+ After a field extension, the columns of $D$ and finitely many paired
172
+ responses span $\mathcal T_P$. These responses can be taken at
173
+ independent small generic partner points, whose sizes need not be
174
+ equal.
175
+ \end{lemma}
176
+
177
+ \begin{proof}
178
+ For the first assertion, apply any $\Omega_P$-linear functional
179
+ annihilating $\mathcal T_P$ to the formal tuple $m$. The result is
180
+ zero. Multiply by the finitely many determinants of
181
+ $W(Q)-\lambda_h$ that occur. The cleared expression is a finite
182
+ sum of products of base-point scalars and matrix-entry series; its
183
+ auxiliary coefficients have a uniform valuation bound. Its formal
184
+ identity is therefore equivalent to its identity at a small generic
185
+ partner, by Lemma~\ref{lem:generic-detection}. It persists under the
186
+ admissible specializations of Lemma~\ref{lem:admissible-evaluation}.
187
+ Divide by the specialized determinants when they are nonzero. The
188
+ same argument, entry by entry, proves the scalar identities for
189
+ $M_h$. It also proves the projected assertion, without introducing
190
+ any spectral labels for the partner input.
191
+
192
+ Choose finitely many coefficient vectors, together with columns of
193
+ $D$, that span $\mathcal T_P$, and select a nonzero minor witnessing
194
+ their rank. For each column requiring a partner, use a separate set
195
+ of partner variables. By multilinearity, the corresponding
196
+ determinant of the series columns has that nonzero minor as the
197
+ coefficient of a specified product of monomials. It is therefore a
198
+ nonzero formal series. Clear the column denominators. The numerator
199
+ is still nonzero, and its coefficients are uniformly bounded below
200
+ in valuation. Independent small generic evaluations keep this
201
+ numerator and its denominators nonzero, by
202
+ Lemma~\ref{lem:generic-detection}. The resulting values attain the
203
+ full dimension. The first assertion places all of them in the
204
+ extended active space.
205
+
206
+ This argument evaluates cleared numerators, not the possibly
207
+ divergent geometric expansions of their inverses. The distinction
208
+ is precisely the one made in Section~\ref{subsec:formal-conventions}.
209
+ \end{proof}
210
+
211
+ The lemma also applies after adjoining Taylor or Laurent parameters.
212
+ One first clears determinants and then works coefficientwise as in
213
+ Lemma~\ref{lem:admissible-evaluation}. In particular, it permits
214
+ triangular partners with repeated base blocks, provided the inverses
215
+ required for the selected target roots exist in the chosen Laurent
216
+ field.
217
+
218
+ \subsection{A partition of the eigenvalue labels}
219
+ \label{subsec:active-partition}
220
+
221
+ The active space has a stronger structure than a general linear
222
+ subspace. Its coordinates form groups whose responses are always in
223
+ a fixed ratio.
224
+
225
+ \begin{proposition}\label{prop:active-partition}
226
+ For the direction $v$ chosen in \eqref{eq:nonzero-direction}, there
227
+ is a partition of $\{1,\ldots,e_n\}$ such that
228
+ \[
229
+ \mathcal T_P=
230
+ \left\{c\in\Omega_P^{e_n}:
231
+ \frac{c_h}{D_h(P;v)}\text{ is constant on each part}\right\}.
232
+ \]
233
+ \end{proposition}
234
+
235
+ \begin{proof}
236
+ We first prove that $\mathcal T_P$ is closed under the operation
237
+ \begin{equation}
238
+ (a,b)\longmapsto
239
+ \left(\frac{a_hb_h}{D_h(P;v)}\right)_h.
240
+ \label{eq:weighted-product}
241
+ \end{equation}
242
+ Choose two finite spanning sets supplied by
243
+ Lemma~\ref{lem:active-specialization}, using independent partner
244
+ points for the two sets. It suffices to prove the assertion for a
245
+ column $a$ in the first set and a column $b$ in the second, over their
246
+ joint coefficient field $E$.
247
+
248
+ Put $P'=P+\xi v$. Use a triangular chain with endpoints $P,P$,
249
+ middle point $P'$, an optional point $Q_1$ between the first endpoint
250
+ and $P'$, and an optional point $Q_2$ between $P'$ and the last
251
+ endpoint. A direct step represents a loop column; an excursion
252
+ through $Q_i$ represents a paired column. Put the arrows defining
253
+ $a$ and $b$ on the successive steps, with no other input arrows.
254
+ Group the internal positions as a single partner $C(\xi)$. Its
255
+ size belongs to $\mathcal S$.
256
+
257
+ For every target label, $W(C(\xi))-\lambda_h$ is invertible over
258
+ $E((\xi))$. The optional blocks have spectra disjoint from $P$.
259
+ At the middle block, the branch reducing to $\lambda_h$ moves with
260
+ nonzero derivative $D_h(P;v)$; all other branches are already away
261
+ from $\lambda_h$. Thus
262
+ \begin{equation}
263
+ \left.\xi\bigl(W(P')-\lambda_h\bigr)^{-1}\right|_{\xi=0}
264
+ =\frac{\pi_h}{D_h(P;v)}.
265
+ \label{eq:middle-residue}
266
+ \end{equation}
267
+ This follows directly by scalar branch separation.
268
+
269
+ By Lemma~\ref{lem:active-specialization}, the paired response through
270
+ $C(\xi)$ belongs to $\mathcal T_P\otimes E((\xi))$. Eliminate
271
+ the optional blocks first in its Schur formula. Triangularity means
272
+ that their elimination does not change the middle diagonal block.
273
+ All terms are regular at $\xi=0$ except the middle inverse in
274
+ \eqref{eq:middle-residue}. The effective first-to-middle coupling,
275
+ compressed by $\pi_h$ at both ends and evaluated at zero, is
276
+ $a_h\pi_h$. For a direct step this is
277
+ \eqref{eq:loop-response}; for an excursion it is
278
+ \eqref{eq:paired-response}. The corresponding middle-to-last
279
+ coupling is $b_h\pi_h$.
280
+
281
+ The singular term occurs with the minus sign in the Schur
282
+ complement. Multiplying by $\xi$ and reducing at zero therefore
283
+ gives
284
+ \[
285
+ \left(-\frac{a_hb_h}{D_h(P;v)}\right)_h
286
+ \in\mathcal T_P\otimes E.
287
+ \]
288
+ Taking a Laurent coefficient preserves membership in this fixed
289
+ finite dimensional space: apply its annihilating linear functionals.
290
+ Bilinearity and the two spanning sets prove closure under
291
+ \eqref{eq:weighted-product} after extension to $E$, and faithful
292
+ scalar extension proves it over $\Omega_P$.
293
+
294
+ Divide coordinates by the nowhere-zero vector $D(P;v)$. The resulting
295
+ space $\mathcal U\subseteq\Omega_P^{e_n}$ contains $1$, since
296
+ $D(P;v)\in\mathcal T_P$, and is closed under coordinatewise
297
+ multiplication. Declare two coordinates equivalent if every element
298
+ of $\mathcal U$ has the same value on them. By avoiding finitely
299
+ many proper linear subspaces, choose an element of $\mathcal U$
300
+ whose values distinguish all the equivalence classes. Lagrange
301
+ interpolation in this element gives the indicator function of each
302
+ class. These indicators span all class-constant functions. Thus
303
+ $\mathcal U$ is exactly that algebra of functions, proving the
304
+ proposition.
305
+ \end{proof}
306
+
307
+ We call two labels in the same part \emph{linked}. The number of
308
+ parts is $a_n$. Selecting one representative from each part
309
+ identifies $\mathcal T_P$ with the full coordinate space on those
310
+ representatives. The next stage must show that these response
311
+ relations control higher-order free-letter errors, rather than only
312
+ the two elementary perturbations used to define them.
preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/build/sections/transfer.tex ADDED
@@ -0,0 +1,250 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Transfer of the first unsolved word coefficient}
2
+ \label{sec:word-transfer}
3
+
4
+ Our next objective is to control equations in free letters. The first and
5
+ paired responses describe matrix perturbations with one loop or two opposite
6
+ arrows. We show that they also contain the first unsolved coefficient of an
7
+ arbitrary free-series perturbation. The argument unfolds a word along a
8
+ triangular chain and then replaces its internal states by a single auxiliary
9
+ partner. The only difficulty is that this partner initially has the target
10
+ eigenvalue. The following linear-algebra observation explains how to remove
11
+ that singularity without changing the coefficient being computed.
12
+
13
+ \begin{lemma}[An inverse between two vanishing couplings]
14
+ \label{lem:killed-pole}
15
+ Let $E$ be a field and let $M(\xi)\in\operatorname{End}_E(V)[[\xi]]$, where
16
+ $V$ is finite dimensional. Suppose that zero is a semisimple eigenvalue of
17
+ $M_0=M(0)$, and let $\Pi$ be its spectral projection. Suppose that
18
+ \[
19
+ G=\Pi M'(0)\Pi\big|_{\ker M_0}
20
+ \]
21
+ is invertible. Then $M(\xi)^{-1}$ exists over $E((\xi))$ and has a pole of
22
+ order at most one. Let $J$ be zero on $\ker M_0$ and equal to $M_0^{-1}$ on
23
+ $\operatorname{im}M_0$. If $L(\xi)$ and $B(\xi)$ are compatible matrix
24
+ series satisfying
25
+ \[
26
+ L(0)\Pi=0,\qquad \Pi B(0)=0,
27
+ \]
28
+ then
29
+ \begin{equation}
30
+ \label{eq:killed-pole-limit}
31
+ \lim_{\xi\to0}L(\xi)M(\xi)^{-1}B(\xi)=L(0)JB(0).
32
+ \end{equation}
33
+
34
+ Suppose additionally that $e$ is an idempotent, $f=1-e$,
35
+ $fM_0f$ is invertible on $fV$, and $e:\ker M_0\to eV$ is an isomorphism.
36
+ Under the same two coupling conditions,
37
+ \begin{equation}
38
+ \label{eq:fixed-complement-inverse}
39
+ L(0)JB(0)=L(0)f(fM_0f)^{-1}fB(0).
40
+ \end{equation}
41
+ \end{lemma}
42
+
43
+ \begin{proof}
44
+ Use $V=\ker M_0\oplus\operatorname{im}M_0$. In this decomposition
45
+ \[
46
+ M(\xi)=
47
+ \begin{pmatrix}
48
+ \xi G+O(\xi^2)&O(\xi)\\
49
+ O(\xi)&M_0|_{\operatorname{im}M_0}+O(\xi)
50
+ \end{pmatrix}.
51
+ \]
52
+ The lower-right block is invertible and the Schur complement of that block
53
+ is $\xi G+O(\xi^2)$. The upper-left block of $M(\xi)^{-1}$ is consequently
54
+ $\xi^{-1}G^{-1}+O(1)$; its off-diagonal blocks are bounded; and its
55
+ lower-right block tends to $M_0^{-1}|_{\operatorname{im}M_0}$.
56
+ The kernel components of both couplings are $O(\xi)$. Multiplying these
57
+ four blocks proves \eqref{eq:killed-pole-limit}.
58
+
59
+ For the second assertion, write $b=B(0)u$. The condition $\Pi b=0$ places
60
+ $b$ in $\operatorname{im}M_0$. Solutions of $M_0x=b$ differ by
61
+ $\ker M_0$. Since projection to $eV$ is an isomorphism on that kernel,
62
+ there is a unique solution with $ex=0$. Its $f$ coordinate is
63
+ $(fM_0f)^{-1}fb$. All solutions have the same image under $L(0)$ because
64
+ $L(0)$ kills $\ker M_0$. Comparing this solution with $Jb$ proves
65
+ \eqref{eq:fixed-complement-inverse}.
66
+ \end{proof}
67
+
68
+ We now recall exactly which response identities enter the transfer
69
+ argument. At a small generic point $P$ of size $n\in\mathcal S$, the
70
+ eigenvalues $\lambda_h$ have projections $\pi_h$ of rank $t$. The first
71
+ response is $D_h(P;Y)\pi_h$. A pair of arrows through an independent
72
+ partner $Q$ gives $m_h(P,Q;U,V)\pi_h$. The columns of the first responses
73
+ and the coefficient vectors of all these paired responses span
74
+ $\mathcal T_P$. By Lemma~\ref{lem:active-specialization}, their scalarity
75
+ and all linear containment identities persist for a block-triangular
76
+ partner after its finitely many resolvent determinants are cleared. For a
77
+ set of target labels $I$, only the determinants belonging to labels in $I$
78
+ are needed. We use the notation
79
+ \[
80
+ \mathcal T_P|_I=\{(c_h)_{h\in I}:(c_h)_h\in\mathcal T_P\}.
81
+ \]
82
+ These spaces and identities are extended to the coefficient field in use.
83
+ We also fix a direction $v$ with $D_h(P;v)\ne0$ for every target label.
84
+
85
+ \begin{proposition}[Transfer of a leading coefficient]
86
+ \label{prop:word-transfer}
87
+ Let $R=\operatorname{diag}(P,C_0)$ be a small matrix input of total size $N\in
88
+ \mathcal S$;
89
+ the block $C_0$ may be absent. Let $I$ be a set of labels at
90
+ $P$ such that $W(C_0)-\lambda_h$ is invertible for every $h\in I$.
91
+ Work over a field $E$ containing the labeled spectral data at $P$ and the
92
+ entries of $C_0$, with the formal evaluations allowed by
93
+ Lemma~\ref{lem:admissible-evaluation}. Let
94
+ \[
95
+ Z(s_1,s_2)\in M_N(E)\langle\!\langle s_1,s_2\rangle\!\rangle^2
96
+ \]
97
+ have constant term $R$. These are input matrices: their scalar entries
98
+ act on the input factor and commute with the old coefficient algebra.
99
+
100
+ For $h\in I$, embed $\pi_h$ at the $P$ block, put $\bar\pi_h=1-\pi_h$,
101
+ and form
102
+ \[
103
+ S_h(Z)=\pi_h(W(Z)-\lambda_h)\pi_h
104
+ -\pi_hW(Z)\bar\pi_h
105
+ \bigl(\bar\pi_h(W(Z)-\lambda_h)\bar\pi_h\bigr)^{-1}
106
+ \bar\pi_hW(Z)\pi_h.
107
+ \]
108
+ Suppose that every $S_h(Z)$ vanishes in degrees less than $\ell$, where
109
+ $\ell\ge1$. For each word $\omega$ of length $\ell$, there are scalars
110
+ $c_{h,\omega}\in E$ such that
111
+ \[
112
+ [S_h(Z)]_\omega=c_{h,\omega}\pi_h,
113
+ \qquad (c_{h,\omega})_{h\in I}\in
114
+ (\mathcal T_P|_I)\otimes E.
115
+ \]
116
+ The same conclusion holds for homogeneous degree-$\ell$ coefficients of
117
+ perturbations in finitely many ordinary commuting parameters.
118
+ \end{proposition}
119
+
120
+ \begin{proof}
121
+ For $\ell=1$, only the $P$-to-$P$ input coefficient contributes to the
122
+ compressed derivative, so the assertion is the first-response identity.
123
+ Assume $\ell\ge2$ and fix a word $\omega$ of length $\ell$.
124
+
125
+ \paragraph{Unfolding the word.}
126
+ Use $\ell+1$ ordered states. On consecutive steps put the letters of
127
+ $\omega$, and evaluate a word by following that path. Thus a coefficient
128
+ of $Z$ for a substring becomes the corresponding strictly upper block of
129
+ the input, while every diagonal block is $R$. The $(1,\ell+1)$ block
130
+ extracts precisely the coefficient of $\omega$. This substitution is a
131
+ homomorphism on the free-series ring modulo degree $\ell+1$, and it
132
+ therefore respects every inverse with invertible constant term.
133
+
134
+ Keep only $P$ at the two endpoint states, leaving all $R$ blocks at the
135
+ $\ell-1$ internal states. This operation does not change the required
136
+ compressed endpoint coefficient. At an endpoint, constant input steps
137
+ preserve the blocks $P,C_0$, and the constant output commutes with
138
+ $\pi_h$. A contributing Schur path can therefore neither enter the
139
+ first endpoint complement from its target projection nor leave the last
140
+ endpoint complement for its target projection. All complement
141
+ eliminations relevant to the coefficient occur at internal states.
142
+
143
+ Denote the internal input by $Q_0$. Its size is $(\ell-1)N$ and hence
144
+ belongs to $\mathcal S$. Grouping the internal
145
+ states, write the cropped input as
146
+ \[
147
+ T_0=\begin{pmatrix}
148
+ P&G_1&Y\\0&Q_0&G_2\\0&0&P
149
+ \end{pmatrix}.
150
+ \]
151
+ Here each entry denotes a pair of input matrices. In the output write
152
+ $E_1=W(T_0)_{12}$, $E_2=W(T_0)_{23}$, and $F=W(T_0)_{13}$.
153
+
154
+ \paragraph{The internal target eigenspace.}
155
+ Fix $h\in I$, set $M_0=W(Q_0)-\lambda_h$, and let $e$ be the sum of the
156
+ fixed copies of $\pi_h$ on its internal states. Put $f=1-e$.
157
+ The matrix $fM_0f$ is upper triangular with invertible diagonal blocks.
158
+ Moreover its Schur complement on $eV$ is zero: every strictly upper
159
+ coefficient is a coefficient for a proper substring of $\omega$, and
160
+ these vanish by hypothesis. Its kernel is consequently the graph
161
+ \[
162
+ u\longmapsto u-f(fM_0f)^{-1}fM_0e u,
163
+ \qquad u\in eV.
164
+ \]
165
+ Projection onto $eV$ is an isomorphism on this kernel, whose dimension is
166
+ $(\ell-1)t$. Triangularity shows that this is also the full algebraic
167
+ multiplicity of zero. Thus zero is semisimple. Let $\Pi$ be its
168
+ spectral projection.
169
+
170
+ The same argument applies to the chain consisting of the first endpoint
171
+ and the internal states, and to the chain consisting of the internal
172
+ states and the last endpoint. They involve only proper substrings.
173
+ Solving their triangular kernel equations shows that the couplings
174
+ between their zero eigenspaces vanish:
175
+ \begin{equation}
176
+ \label{eq:transfer-coupling-annihilation}
177
+ \pi_hE_1\Pi=0,\qquad \Pi E_2\pi_h=0.
178
+ \end{equation}
179
+ Indeed any nonzero compressed coupling would reduce the kernel dimension
180
+ below the sum of the diagonal zero multiplicities. This argument uses
181
+ semisimplicity only at the target eigenvalue.
182
+
183
+ \paragraph{A regularized auxiliary partner.}
184
+ In every internal copy of $R$, replace its $P$ block by $P+\xi v$, keeping
185
+ all arrows fixed; call the resulting input $Q(\xi)$. Put
186
+ $M(\xi)=W(Q(\xi))-\lambda_h$.
187
+ The spectral projection $\Pi$ is upper triangular in the state order,
188
+ with diagonal equal to the fixed target projections. The graph
189
+ identification of its range with $eV$ is upper triangular with identity
190
+ diagonal. It follows that
191
+ \[
192
+ \Pi M'(0)\Pi\big|_{\ker M_0}
193
+ \]
194
+ is upper triangular in this identification, with every diagonal block
195
+ equal to $D_h(P;v)I_t$. It is therefore invertible. This verifies the
196
+ simple-pole hypothesis of Lemma~\ref{lem:killed-pole}, including the
197
+ effect of all internal triangular arrows.
198
+
199
+ Let $T(\xi)$ be the corresponding full cropped input and use $E_1(\xi)$,
200
+ $E_2(\xi)$, $F(\xi)$ for its output blocks. For nonzero formal $\xi$, the
201
+ compressed endpoint expression is
202
+ \begin{align}
203
+ \mathcal E_h(\xi)
204
+ &=\pi_h\bigl(F(\xi)-E_1(\xi)M(\xi)^{-1}E_2(\xi)\bigr)\pi_h
205
+ \label{eq:transfer-regularized-expression}\\
206
+ &=D_h(P;Y)\pi_h+M_h(P,Q(\xi);G_1,G_2).
207
+ \nonumber
208
+ \end{align}
209
+ Its tuple is scalar and belongs to the projected active space over
210
+ $E((\xi))$. This is exactly the specialized paired-response identity:
211
+ the auxiliary block is upper triangular, its diagonal entries are small
212
+ blocks with a Taylor shift, and its strictly upper entries are fixed
213
+ finite matrices. Clear the target resolvent determinants first and
214
+ apply Lemma~\ref{lem:active-specialization}; restore the inverses over
215
+ $E((\xi))$, where the preceding argument proves they exist. No
216
+ specialization of an undefined inverse is being used.
217
+
218
+ \paragraph{Identifying the limit.}
219
+ By \eqref{eq:transfer-coupling-annihilation} and
220
+ Lemma~\ref{lem:killed-pole}, expression
221
+ \eqref{eq:transfer-regularized-expression} has the finite limit
222
+ \[
223
+ \pi_h\bigl(F-E_1JE_2\bigr)\pi_h
224
+ =\pi_h\bigl(F-E_1f(fM_0f)^{-1}fE_2\bigr)\pi_h.
225
+ \]
226
+ The last expression eliminates precisely the fixed complementary
227
+ spaces in the internal states. By the unfolding and endpoint-cropping
228
+ argument it is $[S_h(Z)]_\omega$. In particular the limiting inverse has
229
+ not changed the coefficient to one computed with a different choice of
230
+ complement. Taking the limit in the scalar-response identities and in
231
+ the finitely many linear equations defining $\mathcal T_P|_I$ proves
232
+ the assertion simultaneously for all target labels.
233
+
234
+ Finally consider a perturbation in commuting variables $h_1,\ldots,h_s$.
235
+ Substitute $h_j=a_jz$ for arbitrary scalar directions $a_j$ and one free
236
+ letter $z$. The lower homogeneous terms still vanish, so the result
237
+ just proved applies to the degree-$\ell$ coefficient on every such
238
+ line. Scalarity and containment in a fixed finite-dimensional linear
239
+ space are linear conditions. Each of their annihilators therefore
240
+ gives a homogeneous polynomial in the $a_j$ that vanishes identically.
241
+ Over the infinite characteristic-zero field all its coefficients vanish.
242
+ This proves the commuting-parameter assertion.
243
+ \end{proof}
244
+
245
+ Proposition~\ref{prop:word-transfer} is the bridge from responses to
246
+ free-series equations. It controls a first unsolved coefficient without
247
+ assuming that the perturbation is commutative or that the auxiliary
248
+ matrix has a separated spectrum before regularization. We next use its
249
+ commuting-parameter consequence to show that linked responses arise from
250
+ actual formal relations between eigenvalues.
preprints/A-Counterexample-to-Kuroshs-Division-Ring-Problem-September-23-2026/paper.pdf ADDED
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+ version https://git-lfs.github.com/spec/v1
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preprints/A-Counterexample-to-Rysers-Covering-Conjecture-September-23-2026/README.md ADDED
@@ -0,0 +1,18 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ # [A counterexample to Ryser's covering conjecture](paper.pdf)
2
+
3
+ **Author:** OpenAI
4
+
5
+ **Date:** September 23, 2026
6
+
7
+ ## Citation
8
+
9
+ ```bibtex
10
+ @misc{OAI:A-Counterexample-to-Rysers-Covering-Conjecture-September-23-2026,
11
+ author = {{OpenAI}},
12
+ title = {{A counterexample to Ryser's covering conjecture}},
13
+ howpublished = {OpenAI Math Release preprint
14
+ \href{https://github.com/openai/math/blob/main/preprints/A-Counterexample-to-Rysers-Covering-Conjecture-September-23-2026/paper.pdf}{OAI:A-Counterexample-to-Rysers-Covering-Conjecture-September-23-2026}},
15
+ year = {2026}
16
+ }
17
+ ```
18
+
preprints/A-Counterexample-to-Rysers-Covering-Conjecture-September-23-2026/build/construction.tex ADDED
@@ -0,0 +1,857 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \Needspace{14\baselineskip}
2
+ \section{A configuration with two coordinatizations}
3
+ \label{sec:gadget}
4
+
5
+ We now use the deletion lemma to construct the exceptional configuration.
6
+ We need two properties of the same set: many points on each undeleted
7
+ line, and rigidity of its small line covers. A change of coordinates
8
+ lets us obtain both. In the original coordinates we delete one line
9
+ in every finite nonzero direction. After the change of coordinates,
10
+ the deleted sets become curves, so the line-survival conclusion of
11
+ Lemma~\ref{lem:linecover} applies to every line. It will force every
12
+ small mixed cover by lines and individual points to be a parallel class.
13
+
14
+ \begin{lemma}
15
+ \label{lem:gadget}
16
+ For every sufficiently large prime \(s\equiv2\pmod3\), there is
17
+ a set \(Y\subseteq\F_s^2\) with the following properties. For each
18
+ \(d\in\F_s^*\), there is an affine line \(\ell_d\) of slope \(d\),
19
+ and
20
+ \[
21
+ Y=\F_s^2\setminus\bigcup_{d\in\F_s^*}\ell_d.
22
+ \]
23
+ For each \(d\in\F_s^*\), every line of slope \(d\) other than
24
+ \(\ell_d\) contains at least five points of \(Y\). The map
25
+ \[
26
+ f:\F_s^2\longrightarrow\F_s^2,
27
+ \qquad f(x,y)=(x^3,y),
28
+ \]
29
+ is a bijection, and every affine line contains at least \(s/8\) points
30
+ of \(f(Y)\). Moreover, if \(a\) affine lines and \(b\) individual
31
+ points cover \(f(Y)\), and
32
+ \begin{equation}
33
+ \label{con-weighted-budget}
34
+ a+\frac b2\le s,
35
+ \end{equation}
36
+ then \(a=s\), \(b=0\), and the lines form a full parallel class.
37
+ Consequently every such mixed cover has weighted cost at least \(s\),
38
+ and no cover of \(f(Y)\) by at most \(s\) lines contains two
39
+ nonparallel lines.
40
+ \end{lemma}
41
+
42
+ \begin{proof}
43
+ Let \(s\) tend to infinity through primes congruent to \(2\pmod3\).
44
+ Since
45
+ \(\gcd(3,s-1)=1\), cubing permutes \(\F_s^*\) and fixes zero.
46
+ Thus \(f\) is bijective. It maps horizontal lines to horizontal
47
+ lines and vertical lines to vertical lines. We first prove the two
48
+ survival properties simultaneously with high probability, then use
49
+ them to classify mixed covers satisfying~\eqref{con-weighted-budget}.
50
+
51
+ \paragraph{Survivors in the original coordinates.}
52
+ Choose the lines \(\ell_d\), independently for the \(s-1\) values
53
+ of \(d\), uniformly within their parallel classes. Fix a line
54
+ \(\ell\) of finite nonzero slope \(d\), and temporarily ignore the
55
+ choice \(\ell_d\). Each of the other \(s-2\) choices deletes a
56
+ uniformly distributed point of \(\ell\). Let \(Z_\ell\) count
57
+ the surviving points on \(\ell\). Its expectation is
58
+ \[
59
+ \mu:=\E Z_\ell=s(1-1/s)^{s-2}.
60
+ \]
61
+ Changing one of these choices changes the survivor count by at most
62
+ two. Apply the independent-trial jump bound and bounded-drift
63
+ concentration estimate of
64
+ \cite[Lemmas~A.2--A.3]{OpenAI2026Balanced} to the exposure martingale,
65
+ with \(T=s-2\), \(L=2\), and \(u=\mu/2\). The martingale has
66
+ zero drift, and hence
67
+ \[
68
+ \Pr(Z_\ell<\mu/2)
69
+ \le 2\exp\left(-\frac{\mu^2}{128(s-2)}\right)
70
+ =\exp(-\Omega(s)).
71
+ \]
72
+ There are fewer than \(s^2\) lines under consideration. A union
73
+ bound, together with \(\mu/2\ge5\) for sufficiently large \(s\),
74
+ shows that all these counts are at least five with probability tending
75
+ to one. If \(\ell\ne\ell_d\), reinstating the deletion by
76
+ \(\ell_d\) changes no point on \(\ell\), since the two lines are
77
+ parallel. Thus every required line in the original coordinates has
78
+ at least five points of \(Y\).
79
+
80
+ \paragraph{Survivors and almost-pencil covers in the new coordinates.}
81
+ In the new coordinates, the possible deletion shapes are
82
+ \[
83
+ F_{d,z}=\{(x^3,dx+z):x\in\F_s\},
84
+ \qquad d\in\F_s^*,\quad z\in\F_s.
85
+ \]
86
+ There are \(s(s-1)\) such shapes, each of size \(s\), and each of
87
+ the \(s-1\) independent trials chooses one of them. Every point
88
+ is deleted by a specified trial with probability \(1/s\), so its
89
+ overall survival probability is the uniform value
90
+ \[
91
+ \delta_s=(1-1/s)^{s-1}\ge\frac14
92
+ \]
93
+ for all sufficiently large \(s\).
94
+
95
+ Each shape meets every affine line in at most three points. For a
96
+ vertical line this follows from bijectivity of cubing; for a
97
+ horizontal line it follows from \(d\ne0\). For a line of finite
98
+ nonzero slope \(m\), the intersection is determined by
99
+ \[
100
+ dx+z=mx^3+u,
101
+ \]
102
+ a nonzero polynomial equation of degree three. In particular, no
103
+ shape is itself a line when \(s>5\). All the hypotheses of
104
+ Lemma~\ref{lem:linecover} hold with field size \(s\), a fixed
105
+ integer constant, for example \(D=3\), survival lower bound
106
+ \(\delta=1/4\), and \(\rho_0=1/100\). The exact-line
107
+ occurrence probabilities are zero, and the subfield restriction is
108
+ automatic for a prime field. With probability tending to one, every
109
+ line consequently contains at least \(s/8\) points of \(f(Y)\),
110
+ and its almost-cover conclusion holds for \(f(Y)\) as well. We now
111
+ combine that conclusion with the lower bound on every line to replace
112
+ an almost pencil by a complete one.
113
+
114
+ \paragraph{From an almost pencil to a full parallel class.}
115
+ Assume these events hold, and consider a cover satisfying
116
+ \eqref{con-weighted-budget}. Repeated resources can be removed;
117
+ alternatively, one may keep their original counts, since removal
118
+ only reduces the budget. The line portion has at most \(s\)
119
+ distinct lines and leaves at most \(b\le2s\) points of \(f(Y)\)
120
+ uncovered. Lemma~\ref{lem:linecover} supplies at least
121
+ \((1-\rho_0)s\) distinct lines in this portion through a common
122
+ projective point \(p\). There are at most \(\rho_0s\) other
123
+ lines, and
124
+ \[
125
+ b\le2(s-a)\le2\rho_0s.
126
+ \]
127
+ If an affine line through \(p\) were absent from the cover, all the
128
+ chosen lines through \(p\) would cover at most one of its affine
129
+ points. The other lines would cover at most \(\rho_0s\) further
130
+ points, and the individual point resources at most \(2\rho_0s\).
131
+ Thus at most \(1+3\rho_0s\) points of this missing line would be
132
+ covered. For sufficiently large \(s\), this contradicts
133
+ \[
134
+ \frac s8>1+3\rho_0s.
135
+ \]
136
+ Every affine line through \(p\) must therefore be present. A
137
+ finite \(p\) requires \(s+1\) lines, which is impossible. An
138
+ infinite \(p\) requires all \(s\) lines in its parallel class,
139
+ and then \eqref{con-weighted-budget} forces \(a=s\) and \(b=0\).
140
+ This also rules out repetitions in a cover attaining the budget.
141
+
142
+ The events used in the two coordinate systems hold simultaneously
143
+ with probability tending to one. Consequently every sufficiently
144
+ large prime \(s\equiv2\pmod3\) admits a successful configuration
145
+ \(Y\). A mixed cover of cost less than
146
+ \(s\) would satisfy \eqref{con-weighted-budget} but not its
147
+ necessary equality conclusion. The two stated consequences follow.
148
+ \end{proof}
149
+
150
+ There are arbitrarily large primes congruent to \(2\pmod3\). Indeed,
151
+ if the list were finite and its product were \(P\), the integer
152
+ \(3P-1\equiv2\pmod3\) would have a prime factor congruent to
153
+ \(2\pmod3\), and none of the primes dividing \(P\) could divide it.
154
+ Fix any sufficiently large prime \(s\equiv2\pmod3\), and choose
155
+ \(Y\) and the omitted lines from Lemma~\ref{lem:gadget}.
156
+ These data remain fixed for the rest of the proof.
157
+
158
+ \section{Ambient placement}
159
+ \label{sec:placement}
160
+
161
+ We will place copies of \(Y\) in a larger affine plane, assign each
162
+ copy the directions in which its labels will change, and delete the
163
+ ambient lines of those directions that meet it. The placement must
164
+ meet two requirements. Joins between different copies must avoid
165
+ their changed directions, while the undeleted points must retain the
166
+ pencil and line-survival properties of Lemma~\ref{lem:linecover}.
167
+ We first specify the copies and direction sets, then prove the
168
+ deletion estimates for independent pools of translates, and finally
169
+ select one compatible translate from each pool.
170
+
171
+ \subsection{Fields, copies, and direction sets}
172
+
173
+ Let \(n\ge3\) be odd, and put \(q=s^n\). We identify \(\F_s\)
174
+ with the prime subfield of \(\F_q\). If \(E\) is a subfield, then
175
+ \(|E|=s^a\), where \(a=[E:\F_s]\), and multiplication of vector-space
176
+ bases gives
177
+ \[
178
+ n=a[\F_q:E].
179
+ \]
180
+ For a proper subfield, the index \([\F_q:E]\) is an odd integer
181
+ larger than one, so it is at least three. Consequently
182
+ \[
183
+ |E|=s^a\le s^{n/3}=q^{1/3}
184
+ \qquad\text{for every proper subfield }E.
185
+ \]
186
+ Thus Theorem~\ref{thm:incidence} and
187
+ Lemma~\ref{lem:linecover} apply along this sequence of ambient
188
+ fields. In this section all constants may depend on the already
189
+ fixed \(s\) and \(Y\), but not on \(n\).
190
+
191
+ The odd-degree condition has now supplied the required subfield bound.
192
+ It remains to assign every ambient direction to at least one copy,
193
+ with bounded overlap between assignments. Identify the ambient
194
+ directions with
195
+ \(\PP^1(\F_q)=\F_q\cup\{\infty\}\), using slope. Choose a
196
+ set \(\Lambda\) of representatives of
197
+ \(\F_q^*/\F_s^*\), with \(1\in\Lambda\). There will be one
198
+ configuration group for each \(\lambda\in\Lambda\), together
199
+ with one further group denoted by \(*\). Write
200
+ \[
201
+ \mathcal I=\Lambda\sqcup\{*\},
202
+ \qquad N_q=|\mathcal I|=\frac{q-1}{s-1}+1.
203
+ \]
204
+ Each index \(i\in\mathcal I\) will specify a pool of translates
205
+ of one configuration. We call this pool a group and will choose one
206
+ translate from each group.
207
+
208
+ For \(\lambda\in\Lambda\), define
209
+ \[
210
+ M_\lambda(x,y)=(x,\lambda y),
211
+ \qquad S_\lambda=\lambda\F_s^*,
212
+ \qquad A_\lambda=\{0,\infty\}.
213
+ \]
214
+ Choose distinct \(u,v\in\F_s^*\) and define
215
+ \[
216
+ M_*=
217
+ \begin{pmatrix}1&1\\u&v\end{pmatrix},
218
+ \qquad
219
+ S_*=(\F_s\cup\{\infty\})\setminus\{u,v\},
220
+ \qquad A_*=\{u,v\}.
221
+ \]
222
+ All these linear maps are invertible. For \(M_*\), the image of
223
+ a finite slope \(t\) is
224
+ \[
225
+ \frac{u+vt}{1+t},
226
+ \]
227
+ where a zero denominator gives the infinite direction. Its images
228
+ of the horizontal and vertical directions are \(u\) and \(v\).
229
+ The induced projective bijection therefore maps the \(s-1\)
230
+ finite nonzero subfield slopes precisely to \(S_*\). The same
231
+ statement for \(M_\lambda\) follows from the slope map
232
+ \(t\mapsto\lambda t\).
233
+
234
+ For each \(i\in\mathcal I\), put
235
+ \[
236
+ W_i=M_i(\F_s^2).
237
+ \]
238
+ The directions of joins of distinct points of \(W_i\) form exactly
239
+ \(S_i\cup A_i\). Each set \(S_i\) has size \(s-1\), and
240
+ \(A_i\) consists of the two images of the coordinate axes. The
241
+ cosets \(S_\lambda\) partition all nonzero finite ambient slopes.
242
+ The extra set \(S_*\) contains \(0\) and \(\infty\). Hence
243
+ every ambient direction belongs to at least one and at most two
244
+ sets \(S_i\). More precisely, the directions belonging to two
245
+ sets are
246
+ \begin{equation}
247
+ \label{con-double-directions}
248
+ S_1\cap S_* = \F_s^*\setminus\{u,v\},
249
+ \end{equation}
250
+ and the two groups involved are always \(1\) and \(*\).
251
+
252
+ The sets \(S_i\) are the directions whose labels will change, and
253
+ \(A_i\) are the images of the two axis directions preserved by \(f\).
254
+ For compatibility between copies we use the
255
+ slightly larger direction sets
256
+ \[
257
+ D_i=
258
+ \begin{cases}
259
+ S_i\cup A_i,&i\in\{1,*\},\\
260
+ S_i,&i\notin\{1,*\}.
261
+ \end{cases}
262
+ \]
263
+ In particular,
264
+ \begin{equation}
265
+ \label{con-conflict-directions}
266
+ D_1=D_*=\PP^1(\F_s),
267
+ \end{equation}
268
+ whereas the remaining \(D_i\) are the nonidentity multiplicative
269
+ cosets of \(\F_s^*\). Every direction occurs in at most two
270
+ sets \(D_i\). Since \(|W_i|=s^2\), \(|D_i|\le s+1\), and
271
+ \(N_q=O_s(q)\), a fixed constant depending only on \(s\)
272
+ satisfies all size and multiplicity assumptions of
273
+ Theorem~\ref{thm:selection}. In a conflict-free selection, including
274
+ the axes in both \(D_1\) and \(D_*\) ensures that an axis line
275
+ meeting one of these two selected copies cannot also meet the other.
276
+ This will enter the weighted cover
277
+ argument for the two groups sharing a direction
278
+ in~\eqref{con-double-directions}.
279
+
280
+ \subsection{Independent candidate pools}
281
+
282
+ Let \(K\) be a fixed pool size supplied by
283
+ Theorem~\ref{thm:selection}. For each
284
+ \(i\in\mathcal I\), choose independent uniform shifts
285
+ \(b_{i,1},\ldots,b_{i,K}\in\F_q^2\), independently between
286
+ groups, and write
287
+ \[
288
+ P_{i,k}=b_{i,k}+W_i,
289
+ \qquad Y_{i,k}=b_{i,k}+M_iY.
290
+ \]
291
+ Associate to this candidate the following set of ambient deletion
292
+ lines:
293
+ \[
294
+ \mathcal B_{i,k}
295
+ =\{\ell:\operatorname{dir}(\ell)\in S_i,
296
+ \ \ell\cap Y_{i,k}\ne\varnothing\}.
297
+ \]
298
+
299
+ \begin{lemma}
300
+ \label{con-deletion-count}
301
+ For every candidate and every \(d\in S_i\), exactly \(s-1\)
302
+ lines of \(\mathcal B_{i,k}\) have direction \(d\). Each of
303
+ these lines contains at least five points of \(Y_{i,k}\).
304
+ Consequently \(|\mathcal B_{i,k}|=(s-1)^2\).
305
+ \end{lemma}
306
+
307
+ \begin{proof}
308
+ Undo the translation and apply \(M_i^{-1}\). An ambient line in
309
+ the given direction meeting \(P_{i,k}\) becomes a line through a
310
+ point of \(\F_s^2\) in a finite nonzero subfield direction. Its
311
+ intersection with \(\F_s^2\) is the corresponding subfield
312
+ line. The \(s\) lines in that subfield parallel class extend to
313
+ distinct parallel ambient lines. Exactly one is the omitted line
314
+ in the definition of \(Y\); the other \(s-1\) each contain at
315
+ least five points of \(Y\), by Lemma~\ref{lem:gadget}. These are
316
+ precisely the lines meeting the candidate's retained configuration.
317
+ \end{proof}
318
+
319
+ Each candidate therefore prescribes a bounded list of deletion lines.
320
+ We next apply the deletion lemma to all these independent lists at
321
+ once. Besides the almost-pencil and line-survival conclusions, we
322
+ need one bound on how many groups a line can meet along joins from an
323
+ external point. All three properties will survive the subsequent
324
+ selection of one candidate per group.
325
+
326
+ \begin{lemma}
327
+ \label{con-pool-properties}
328
+ There are constants \(\delta\in(0,1)\) and
329
+ \(\rho=\delta/10\), independent of \(n\), with the following
330
+ properties with probability tending to one as \(n\) tends to
331
+ infinity through odd integers. Let
332
+ \[
333
+ X_{\rm pool}
334
+ =\F_q^2\setminus
335
+ \bigcup_{i\in\mathcal I}\bigcup_{k=1}^K
336
+ \bigcup_{\ell\in\mathcal B_{i,k}}\ell.
337
+ \]
338
+ \begin{enumerate}
339
+ \item Every cover of \(X_{\rm pool}\) by at most \(q\) affine
340
+ lines contains at least \((1-\rho)q\) lines through a common
341
+ projective point.
342
+ \item For every affine line \(\ell\), if only exact occurrences
343
+ of \(\ell\) are ignored in the pool deletions, at least
344
+ \(\delta q/2\) points of \(\ell\) remain.
345
+ \item For every finite point \(p\) and affine line \(\ell\)
346
+ not through \(p\), at most five groups \(i\) have a candidate
347
+ \(P_{i,k}\) containing a point \(y\in\ell\) whose join to
348
+ \(p\) has direction in \(S_i\).
349
+ \end{enumerate}
350
+ \end{lemma}
351
+
352
+ \begin{proof}
353
+ We verify the hypotheses of Lemma~\ref{lem:linecover} for the full
354
+ pool, which gives the first two assertions. The third follows from
355
+ a separate union bound over finite points and lines.
356
+
357
+ Treat each candidate shift as one independent deletion trial, listing
358
+ the lines of \(\mathcal B_{i,k}\). There are \(KN_q=O_{s,K}(q)\)
359
+ trials, each listing \(m=(s-1)^2\) lines. We may take the shape
360
+ family to be all \(q(q+1)\) ambient affine lines. Each shape has
361
+ size \(q\), and two distinct line shapes intersect in at most one
362
+ point. Thus the shape and trial bounds in
363
+ Lemma~\ref{lem:linecover} hold with a sufficiently large fixed
364
+ integer \(D\) depending only on \(s,K\).
365
+
366
+ A candidate's deleting set is a uniform translate of a fixed union
367
+ of \(m\) lines. Its deletion probability at a fixed point is
368
+ independent of the point and is at most \(m/q\). Independence of
369
+ the shifts makes the overall survival probability \(\delta_q\)
370
+ uniform on \(\F_q^2\). For sufficiently large \(q\),
371
+ \(m/q\le1/2\) and \(N_q\le2q/(s-1)\). Using
372
+ \(\log(1-t)\ge-2t\) for \(0\le t\le1/2\), we obtain
373
+ \[
374
+ \delta_q\ge (1-m/q)^{KN_q}
375
+ \ge \exp\bigl(-2KN_qm/q\bigr)
376
+ \ge \exp\bigl(-4K(s-1)\bigr).
377
+ \]
378
+ Fix
379
+ \(\delta=\exp(-4K(s-1))\) and \(\rho=\delta/10\).
380
+
381
+ For completeness, the exact-line hypothesis also has a uniform
382
+ bound. A fixed line \(\ell\) of direction \(d\) can occur only
383
+ in candidates of groups with \(d\in S_i\), of which there are at
384
+ most two. In each such candidate, there are \(s-1\) translated
385
+ lines in this direction. Each fixed line has probability \(1/q\)
386
+ of becoming \(\ell\) under the uniform shift. Therefore the sum,
387
+ over all trials, of the probabilities of listing \(\ell\) is at
388
+ most
389
+ \begin{equation}
390
+ \label{con-exact-line-probability}
391
+ \frac{2K(s-1)}q.
392
+ \end{equation}
393
+ Increasing the fixed \(D\) if necessary verifies every hypothesis
394
+ of Lemma~\ref{lem:linecover}. Its conclusions give the first two
395
+ properties.
396
+
397
+ To prove the third, fix \(p\notin\ell\). For one candidate in
398
+ group \(i\), there are at most \(s-1\) possible points
399
+ \(y\in\ell\) whose join to \(p\) has a direction in \(S_i\):
400
+ each such direction contributes at most one intersection with
401
+ \(\ell\). A fixed point belongs to a uniform translate of
402
+ \(W_i\) with probability \(s^2/q^2\). The probability for this
403
+ candidate is thus at most
404
+ \[
405
+ \frac{(s-1)s^2}{q^2}.
406
+ \]
407
+ If six distinct groups meet the condition, choose one witnessing
408
+ candidate from each. There are at most \((KN_q)^6=O_{s,K}(q^6)\)
409
+ choices, and their shifts are independent. For the fixed pair
410
+ \((p,\ell)\), the probability of six such groups is therefore
411
+ \(O_{s,K}(q^{-6})\). There are at most
412
+ \(q^2q(q+1)=O(q^4)\) pairs \((p,\ell)\). The union bound gives
413
+ a total failure probability \(O_{s,K}(q^{-2})\), proving the claim.
414
+ \end{proof}
415
+
416
+ \subsection{Selection and transfer of the deletion estimates}
417
+
418
+ The estimates just proved concern independent candidates. We can now
419
+ select compatible copies, using only inclusions to transfer the
420
+ estimates to the selected deletion set.
421
+ By Theorem~\ref{thm:selection}, with probability tending to one the
422
+ same pool admits one candidate per group with no conflicts.
423
+ Intersect this event with those of Lemma~\ref{con-pool-properties}.
424
+ No independence between these events is needed. For every
425
+ sufficiently large odd integer \(n\), their intersection has positive
426
+ probability, so fix a pool in the intersection and a conflict-free
427
+ selection. Denote the selected sets and shifts by
428
+ \[
429
+ P_i=b_i+M_i(\F_s^2),\qquad Y_i=b_i+M_iY.
430
+ \]
431
+ Conflict avoidance gives the useful implication
432
+ \begin{equation}
433
+ \label{con-separation}
434
+ i\ne j,\quad \operatorname{dir}(\ell)\in D_i,\quad
435
+ \ell\cap P_i\ne\varnothing
436
+ \quad\Longrightarrow\quad \ell\cap P_j=\varnothing.
437
+ \end{equation}
438
+ In particular the \(P_i\) are pairwise disjoint: a common point
439
+ would give a zero difference, which belongs to every conflict
440
+ direction, and each \(D_i\) is nonempty.
441
+
442
+ Let \(B\) be the union, as a set of lines, of the deletion lines
443
+ of the selected candidates, and put
444
+ \begin{equation}
445
+ \label{con-selected-survivors}
446
+ X=\F_q^2\setminus\bigcup_{\ell\in B}\ell.
447
+ \end{equation}
448
+ Then \(X\supseteq X_{\rm pool}\). Moreover, if \(\ell\notin B\),
449
+ every selected deletion line belongs to the pool list after all
450
+ exact occurrences of \(\ell\) have been omitted. Hence \(X\)
451
+ contains the survivor set of that modified pool process. This
452
+ inclusion is deterministic: it holds even if \(\ell\) occurs in an
453
+ unselected candidate and even though the selected shifts depend on the
454
+ whole pool. In particular,
455
+ \begin{equation}
456
+ \label{con-selected-line-bound}
457
+ \ell\notin B
458
+ \quad\Longrightarrow\quad |X\cap\ell|\ge\frac{\delta q}{2}.
459
+ \end{equation}
460
+ The third property of Lemma~\ref{con-pool-properties} also remains
461
+ available for the selection, since it was established for all
462
+ candidates in the pool.
463
+
464
+ This completes the placement: the copies are separated, covers of the
465
+ ordinary survivors by at most \(q\) lines contain an almost pencil,
466
+ every undeleted line contains at least \(\delta q/2\) survivors,
467
+ and the bound of five groups remains valid. The order of choices is
468
+ \(s,Y\), then the selection constant and \(K\), then the deletion
469
+ constants \(D,\delta,\rho\), and finally \(q=s^n\).
470
+ Only after fixing these constants do we require \(q=s^n\) to be
471
+ sufficiently large. All further numerical inequalities below involve
472
+ these fixed constants
473
+ and can be imposed by enlarging this final threshold. Thus the
474
+ construction is available for every sufficiently large odd integer
475
+ \(n\), with the same \(s,Y\); its pools and selected shifts may
476
+ depend on \(n\). The constant used for the ambient deletion lemma
477
+ may depend on \(K\), but it changes no hypothesis of the already
478
+ applied selection theorem. A small value of \(\delta\) only increases
479
+ the final lower threshold on \(q\).
480
+
481
+ \section{The hypergraph and its covering number}
482
+ \label{sec:hypergraph}
483
+
484
+ The placement supplies the ordinary points \(X\) and the exceptional
485
+ copies \(Y_i\). We now turn them into edges. Ordinary edges retain
486
+ all their affine-line labels. In an exceptional copy, the directions
487
+ \(S_i\) instead use line labels read from \(f(Y)\); all remaining
488
+ directions retain their ordinary labels. We will first check that
489
+ every pair of edges still meets, then use the rigidity of \(f(Y)\)
490
+ to rule out covers of size \(q\).
491
+
492
+ \subsection{Vertices, edges, and intersection}
493
+
494
+ Set \(r=q+1\). There is one vertex part \(V_d\) for each
495
+ \(d\in\PP^1(\F_q)\). For every ambient affine line \(\ell\)
496
+ of direction \(d\), place an ordinary vertex \(o_\ell\) in
497
+ \(V_d\). If \(d\in S_i\), let \(t_i(d)\in\F_s^*\) be
498
+ the unique subfield direction whose image under \(M_i\) is
499
+ \(d\). For each of the \(s\) subfield affine lines \(L\) of
500
+ direction \(t_i(d)\), place a special vertex \(v_{i,d,L}\) in
501
+ \(V_d\). These subfield lines are read in the new coordinates
502
+ used for \(f(Y)\). All vertices are formal labels, tagged to be
503
+ distinct between parts, between ordinary and special types, and
504
+ between different groups. In particular each \(V_d\) is finite,
505
+ and the parts are pairwise disjoint.
506
+
507
+ Write \(\ell_d(z)\) for the ambient line of direction \(d\)
508
+ through \(z\), and \(L_t(w)\) for the subfield line of direction
509
+ \(t\) through \(w\in\F_s^2\). Each \(x\in X\) defines the
510
+ ordinary edge
511
+ \[
512
+ e_x=\{o_{\ell_d(x)}:d\in\PP^1(\F_q)\}.
513
+ \]
514
+ For each \(i\in\mathcal I\) and \(w\in Y\), put
515
+ \(y_{i,w}=b_i+M_iw\) and define an exceptional edge by selecting,
516
+ in part \(V_d\), the vertex
517
+ \begin{equation}
518
+ \label{con-exceptional-vertex}
519
+ \begin{cases}
520
+ v_{i,d,L_{t_i(d)}(f(w))},& d\in S_i,\\
521
+ o_{\ell_d(y_{i,w})},&d\notin S_i.
522
+ \end{cases}
523
+ \end{equation}
524
+ Denote this edge by \(e_{i,w}\), and let
525
+ \[
526
+ H=\{e_x:x\in X\}\cup
527
+ \{e_{i,w}:i\in\mathcal I,\ w\in Y\}.
528
+ \]
529
+ Thus an exceptional edge changes labels in the assigned directions,
530
+ without introducing any new part. Every edge contains exactly one
531
+ vertex from every part, so \(H\)
532
+ is \((q+1)\)-partite and \((q+1)\)-uniform. It is nonempty,
533
+ because \(Y\ne\varnothing\).
534
+
535
+ Figure~\ref{fig:two-coordinates} shows how to read an exceptional
536
+ edge from its parameter \(w\). The deletion lines were defined from
537
+ its ordinary base point \(y_{i,w}\), while its special labels use
538
+ \(f(w)\). The two axis parallel classes are preserved by \(f\),
539
+ which joins these descriptions in the intersection proof.
540
+
541
+ \begin{figure}[htbp]
542
+ \centering
543
+ \input{figures/two-coordinates}
544
+ \caption{The two label rules for the vertex of \(e_{i,w}\) in part
545
+ \(V_d\). The left branch uses the embedded point \(b_i+M_iw\);
546
+ the right branch uses \(f(w)=(w_1^3,w_2)\) in the small plane.
547
+ For each \(d\in A_i\), two parameters give the same ordinary label
548
+ exactly when their images under \(f\) lie on the same corresponding
549
+ horizontal or vertical line.
550
+ The diagram records maps and label choices, rather than geometric
551
+ positions in the finite plane.}
552
+ \label{fig:two-coordinates}
553
+ \end{figure}
554
+
555
+ \begin{proposition}
556
+ \label{con-intersection}
557
+ The hypergraph \(H\) is intersecting. Furthermore, all the edges
558
+ in its displayed parametrization are distinct.
559
+ \end{proposition}
560
+
561
+ \begin{proof}
562
+ There are four types of pairs, according to whether their edges are
563
+ ordinary or exceptional and, in the latter case, whether their group
564
+ indices agree.
565
+
566
+ Two ordinary edges with distinct base points share the ordinary
567
+ label of their join. Next, an exceptional base point \(y\in Y_i\)
568
+ lies on a deletion line in every direction of the nonempty set
569
+ \(S_i\), so \(y\notin X\). Its join with \(x\in X\) cannot
570
+ have direction in \(S_i\): otherwise that join would be a selected
571
+ deletion line containing \(x\). Its ordinary label therefore
572
+ belongs to both the exceptional edge and \(e_x\).
573
+
574
+ For exceptional edges from distinct groups \(i,j\), the base
575
+ points are distinct by \eqref{con-separation}. That same separation
576
+ condition ensures that their join has direction outside both
577
+ \(D_i\) and \(D_j\), and hence outside \(S_i\cup S_j\).
578
+ The two edges share its ordinary label.
579
+
580
+ Finally, consider \(e_{i,w}\) and \(e_{i,w'}\) with \(w\ne w'\).
581
+ The transformed points \(f(w),f(w')\) are distinct. If their
582
+ join has finite nonzero slope \(t\), the exceptional edges share
583
+ the special label of this subfield line in the part of direction
584
+ \(M_i(t)\). If their join is horizontal or vertical, the relevant
585
+ original coordinates are equal as well, because \(f\) preserves
586
+ these two parallel classes bijectively. The original base points
587
+ then share an ordinary axis-direction label, in a direction of
588
+ \(A_i\). This completes the intersection proof.
589
+
590
+ We also check that the parameters count distinct edges, as required
591
+ when we count exceptional edges below. Two ordinary labels in
592
+ nonparallel directions determine the ordinary base point, so ordinary
593
+ edges are distinct.
594
+ An exceptional edge has special labels and cannot equal an ordinary
595
+ edge. Within one group, the special labels in any two distinct
596
+ directions of \(S_i\) determine \(f(w)\), since the corresponding
597
+ subfield lines are nonparallel. As \(|S_i|=s-1\ge2\), equal
598
+ exceptional edges within a group would imply \(w=w'\). Finally,
599
+ any special label tagged by group \(i\) is absent from every edge
600
+ of a different group. Exceptional edges in distinct groups are
601
+ therefore distinct too.
602
+ \end{proof}
603
+
604
+ \Needspace{14\baselineskip}
605
+ \subsection{Covering vertices in the small-plane coordinates}
606
+
607
+ We identify the positions of the exceptional edges of group \(i\)
608
+ with \(f(Y)\), via \(e_{i,w}\leftrightarrow f(w)\). The action
609
+ of a covering vertex means the subset of these positions whose edges
610
+ contain that vertex. The next lemma translates every such action
611
+ into one of the two resources in Lemma~\ref{lem:gadget}: a subfield
612
+ line or an individual point.
613
+
614
+ \begin{lemma}
615
+ \label{con-label-action}
616
+ Fix a group \(i\).
617
+ \begin{enumerate}
618
+ \item A special vertex of group \(i\) covers the positions on one
619
+ subfield line. A special vertex of another group covers none.
620
+ \item An ordinary vertex of direction in \(S_i\) covers none.
621
+ An ordinary vertex of direction in \(A_i\), if it covers any
622
+ positions, covers them on a single horizontal or vertical line in
623
+ the \(f\) coordinates.
624
+ \item An ordinary vertex of direction outside \(S_i\cup A_i\)
625
+ covers at most one position.
626
+ \end{enumerate}
627
+ In particular, the positions covered by any one vertex are contained
628
+ in a subfield affine line.
629
+ \end{lemma}
630
+
631
+ \begin{proof}
632
+ The assertions for special vertices and altered ordinary directions
633
+ follow directly from \eqref{con-exceptional-vertex}. For an axis
634
+ direction, undoing \(b_i,M_i\) fixes one original coordinate, so
635
+ applying \(f\) gives the corresponding horizontal or vertical
636
+ line. A line in a direction outside \(S_i\cup A_i\) cannot
637
+ contain two points of \(P_i\), since the join directions of that
638
+ embedded subplane are exactly \(S_i\cup A_i\). It therefore
639
+ covers at most one exceptional position. A singleton can be
640
+ included in an arbitrary subfield line through it, and an empty
641
+ set requires no covering resource.
642
+ \end{proof}
643
+
644
+ \subsection{The final cover argument}
645
+
646
+ \begin{proof}[Completion of the proof of Theorem~\ref{thm:main}]
647
+ We prove that \(H\) has no vertex cover of size at most \(q\).
648
+ Suppose to the contrary that \(C\) is such a cover. Its ordinary
649
+ vertices, regarded as affine lines, must cover \(X\): special
650
+ vertices belong to no ordinary edge. These lines also cover
651
+ \(X_{\rm pool}\). Lemma~\ref{con-pool-properties} therefore
652
+ gives a projective point \(p\) such that at least
653
+ \((1-\rho)q\) ordinary vertices of \(C\) are lines through
654
+ \(p\). The line-survival bound will force every undeleted member
655
+ of this pencil into \(C\). We then count the vertices left for
656
+ exceptional edges, separating centers at infinity, centers inside one
657
+ of the sets \(P_i\), and finite centers outside them all.
658
+
659
+ \paragraph{Every undeleted line in this pencil is forced.}
660
+ We claim that
661
+ \begin{equation}
662
+ \label{con-forced-pencil}
663
+ p\in\ell,\quad\ell\notin B
664
+ \quad\Longrightarrow\quad o_\ell\in C,
665
+ \end{equation}
666
+ where incidence with an infinite \(p\) means that \(\ell\) has
667
+ the corresponding direction. If \(o_\ell\) were missing, all
668
+ other lines of \(C\) through \(p\) would cover at most one
669
+ affine point of \(\ell\). There are at most \(\rho q\)
670
+ vertices outside the large pencil subcollection. Each of their
671
+ ordinary lines covers at most one point of \(\ell\), and their
672
+ special vertices cover no ordinary edge. Consequently
673
+ \[
674
+ |X\cap\ell|\le1+\rho q.
675
+ \]
676
+ This contradicts \eqref{con-selected-line-bound}, since
677
+ \(\delta q/2>1+\rho q\) for sufficiently large \(q\) and
678
+ \(\rho=\delta/10\). At infinity the pencil lines are parallel,
679
+ so the possible contribution of one central point is absent; the
680
+ same upper bound still applies.
681
+
682
+ Let \(F_p\) be the set of ordinary vertices forced by
683
+ \eqref{con-forced-pencil}, and call the vertices of \(C\setminus F_p\)
684
+ the additional vertices. The deleted pencil lines determine how
685
+ many additional vertices the assumed budget \(|C|\le q\) permits.
686
+
687
+ \paragraph{An infinite center.}
688
+ Suppose \(p\) is the point at infinity in direction \(d\). Put
689
+ \[
690
+ I_d=\{i\in\mathcal I:d\in S_i\},
691
+ \qquad z=|I_d|\in\{1,2\}.
692
+ \]
693
+ Only these groups contribute deletion lines in direction \(d\),
694
+ and each contributes \(s-1\), by
695
+ Lemma~\ref{con-deletion-count}. At most \(z(s-1)\) of the
696
+ \(q\) lines in this parallel class belong to \(B\). Thus
697
+ \[
698
+ |C\setminus F_p|\le z(s-1).
699
+ \]
700
+ None of the forced vertices covers any exceptional edge of a group
701
+ in \(I_d\), because those groups use special vertices in
702
+ direction \(d\).
703
+
704
+ If \(z=1\), all positions of this group's \(f(Y)\) must therefore
705
+ be covered by at most \(s-1\) additional vertices. By
706
+ Lemma~\ref{con-label-action}, their effects can be included in at
707
+ most \(s-1\) subfield lines. This contradicts
708
+ Lemma~\ref{lem:gadget}.
709
+
710
+ If \(z=2\), the two groups are \(1,*\), by
711
+ \eqref{con-double-directions}. An additional vertex can now meet
712
+ both groups, so we use the weighted line-and-point budget instead of
713
+ counting one line per vertex. For each of these groups let \(a_i\)
714
+ count the additional vertices that cover at least one of its
715
+ positions and are either special vertices of this group or ordinary
716
+ vertices in its axis directions \(A_i\). Let \(b_i'\) count the
717
+ other additional vertices covering a position of the group. By
718
+ Lemma~\ref{con-label-action}, the latter vertices each cover only
719
+ a singleton. The former supply subfield lines. The weighted
720
+ conclusion of Lemma~\ref{lem:gadget} gives
721
+ \begin{equation}
722
+ \label{con-two-group-lower}
723
+ a_i+\frac{b_i'}2\ge s
724
+ \qquad (i=1,*).
725
+ \end{equation}
726
+
727
+ Each additional vertex contributes at most one to the sum of the
728
+ two left sides. A special vertex is confined to its tagged group.
729
+ An ordinary axis-direction vertex counted in \(a_i\) is a line
730
+ meeting \(P_i\) with direction in \(A_i\subseteq D_i\); by
731
+ \eqref{con-separation} it cannot meet the other group's \(P_j\).
732
+ It therefore contributes nothing to that other group, even as a
733
+ singleton. Any vertex of neither exclusive type contributes at
734
+ most \(1/2\) to each group. This accounts for every type of
735
+ additional vertex, including those covering neither group.
736
+ Summing \eqref{con-two-group-lower}, we obtain
737
+ \[
738
+ 2s\le a_1+\frac{b_1'}2+a_*+\frac{b_*'}2
739
+ \le |C\setminus F_p|\le2(s-1),
740
+ \]
741
+ a contradiction.
742
+
743
+ \paragraph{A finite center inside an embedded configuration.}
744
+ Now let \(p\) be finite, and write
745
+ \[
746
+ h_p=|\{\ell\in B:p\in\ell\}|.
747
+ \]
748
+ There are \(q+1\) affine lines through \(p\), so
749
+ \begin{equation}
750
+ \label{con-finite-budget}
751
+ |F_p|=q+1-h_p,
752
+ \qquad |C\setminus F_p|\le h_p-1.
753
+ \end{equation}
754
+ The loss of one in the second inequality comes from the \(q+1\)
755
+ members of a finite pencil and the assumed cover size \(q\).
756
+ If \(h_p=0\), the forced vertices already exceed the permitted
757
+ size of \(C\). We may therefore assume \(h_p\ge1\) in both
758
+ finite-center cases.
759
+
760
+ Suppose \(p\in P_i\), for the necessarily unique such group.
761
+ Every deletion line through \(p\) comes from this group: a line
762
+ from another group would contradict \eqref{con-separation}, since
763
+ its direction belongs to that other group's conflict set. There
764
+ is at most one such line in each direction of \(S_i\), and hence
765
+ \begin{equation}
766
+ \label{con-internal-pencil-size}
767
+ h_p\le s-1.
768
+ \end{equation}
769
+ Let \(w_p=M_i^{-1}(p-b_i)\in\F_s^2\), whether or not
770
+ \(w_p\in Y\). We account for the exceptional positions of this
771
+ group covered by \(F_p\): they will all lie on two nonparallel
772
+ lines in the new coordinates. For a position with base point
773
+ \(y\ne p\), its join with \(p\) has a direction in
774
+ \(S_i\cup A_i\). A direction in \(S_i\) cannot cover this
775
+ edge by an ordinary vertex. Any actual forced coverage must
776
+ therefore lie along one of the two axis-direction lines through
777
+ \(p\). A position based at \(p\) itself, if present, lies on
778
+ both these axes as well.
779
+
780
+ Since \(f\) preserves the two coordinate parallel classes, all
781
+ these covered positions are contained, in the new coordinates, in
782
+ the horizontal and vertical lines through \(f(w_p)\). The
783
+ remaining positions are covered by the additional vertices; each
784
+ can be included in one subfield line by
785
+ Lemma~\ref{con-label-action}. Equations
786
+ \eqref{con-finite-budget} and \eqref{con-internal-pencil-size}
787
+ would thus give a cover of \(f(Y)\) by at most
788
+ \[
789
+ 2+(h_p-1)\le s
790
+ \]
791
+ lines containing the two nonparallel coordinate lines. These
792
+ are legitimate covering resources whether or not their ordinary labels
793
+ belong to \(F_p\): their union contains every position covered by
794
+ \(F_p\). Removing any duplicate replacement lines preserves these
795
+ two distinct lines and can only decrease the count. This contradicts
796
+ Lemma~\ref{lem:gadget}.
797
+
798
+ \paragraph{A finite center outside all embedded configurations.}
799
+ It remains to consider \(p\notin\bigcup_{i\in\mathcal I}P_i\).
800
+ Here we use the five points on each deletion line, rather than the
801
+ small-plane cover obstruction. We will find \(5h_p\) exceptional
802
+ edges missed by \(F_p\), while each additional vertex covers at
803
+ most five of them.
804
+
805
+ Each group contributes at most one deletion line through \(p\).
806
+ Indeed, two distinct such lines cannot be parallel. After undoing
807
+ \(b_i,M_i\), their subfield affine equations have distinct
808
+ subfield directions. Solving these two equations uses a
809
+ nonsingular linear system over \(\F_s\), so their intersection
810
+ lies in \(\F_s^2\). This would place \(p\) in \(P_i\), a
811
+ contradiction. Also, deletion lines from different groups cannot
812
+ coincide, by \eqref{con-separation}.
813
+
814
+ The \(h_p\) deletion lines through \(p\) therefore come from
815
+ \(h_p\) distinct groups. From each such group \(i\), choose five
816
+ distinct points of \(Y_i\) on its contributing line, possible by
817
+ Lemma~\ref{con-deletion-count}. These give \(5h_p\) distinct
818
+ exceptional edges, by Proposition~\ref{con-intersection}. None
819
+ is covered by a forced ordinary vertex: its unique join line to
820
+ \(p\) is precisely its contributing deletion line, whose
821
+ direction is altered for that group.
822
+
823
+ Any one additional vertex covers at most five of these selected
824
+ edges. For a special vertex this follows because it belongs to
825
+ only one group. An ordinary line through \(p\) covers none,
826
+ by the same unique-join and altered-direction argument. Finally,
827
+ let an ordinary vertex \(o_\ell\), with \(\ell\) not through
828
+ \(p\), cover some selected edges. The line \(\ell\) meets each
829
+ contributing line in at most one point, so \(o_\ell\) covers at most
830
+ one selected edge from each contributing group. Every such group
831
+ has a selected point \(y\in Y_i\cap\ell\) whose join to \(p\)
832
+ has direction in \(S_i\). The third part of
833
+ Lemma~\ref{con-pool-properties}, which applies to all candidates
834
+ and hence to the selection, bounds the number of these groups by
835
+ five. This proves the asserted bound for every additional vertex.
836
+
837
+ By \eqref{con-finite-budget}, at most \(h_p-1\) additional
838
+ vertices are available. They can cover at most \(5(h_p-1)\) of
839
+ the \(5h_p\) selected edges, a final contradiction.
840
+
841
+ We have ruled out every possible projective center \(p\), and
842
+ hence every vertex cover of size at most \(q\). Therefore
843
+ \(\tau(H)\ge q+1\). Conversely, any edge of the nonempty
844
+ intersecting hypergraph \(H\) is itself a vertex cover and has
845
+ size \(q+1\). It follows that
846
+ \[
847
+ \tau(H)=q+1.
848
+ \]
849
+ The parameter choices in Section~\ref{sec:placement} give this
850
+ hypergraph for every sufficiently large odd integer \(n\), with
851
+ \(q=s^n\), after fixing any sufficiently large prime
852
+ \(s\equiv2\pmod3\) and a successful \(Y\). Choose one such \(Y\)
853
+ for each eligible \(s\), and let \(n_0(s)\ge3\) exceed all the
854
+ resulting degree thresholds. This proves Theorem~\ref{thm:main}.
855
+ Since there are arbitrarily large odd integers, it also gives infinitely
856
+ many ranks \(r=q+1\).
857
+ \end{proof}
preprints/A-Counterexample-to-Rysers-Covering-Conjecture-September-23-2026/build/figures/two-coordinates.tex ADDED
@@ -0,0 +1,19 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \begin{tikzpicture}[
2
+ >=Latex,
3
+ point/.style={draw,rounded corners=2pt,align=center,inner sep=7pt},
4
+ labelbox/.style={draw,align=center,text width=5.1cm,inner sep=7pt},
5
+ every node/.style={font=\small}]
6
+ \node[point] (w) at (0,0) {$w=(w_1,w_2)\in Y$};
7
+ \node[point] (old) at (-3.5,-1.55)
8
+ {Ambient coordinates\\[3pt]$y_{i,w}=b_i+M_iw\in Y_i$};
9
+ \node[point] (new) at (3.5,-1.55)
10
+ {Small-plane coordinates\\[3pt]$f(w)=(w_1^3,w_2)\in f(Y)$};
11
+ \node[labelbox] (ordinary) at (-3.5,-3.65)
12
+ {Ordinary vertex in $V_d$\\[3pt]$o_{\ell_d(y_{i,w})}$};
13
+ \node[labelbox] (special) at (3.5,-3.65)
14
+ {Special vertex in $V_d$\\[3pt]$v_{i,d,L_{t_i(d)}(f(w))}$};
15
+ \draw[->] (w) -- node[above left,inner sep=2pt,xshift=-4pt,yshift=-2pt] {embed} (old);
16
+ \draw[->] (w) -- node[above right,inner sep=2pt,xshift=4pt,yshift=-2pt] {apply $f$} (new);
17
+ \draw[->] (old) -- node[left] {$d\notin S_i$} (ordinary);
18
+ \draw[->] (new) -- node[right] {$d\in S_i$} (special);
19
+ \end{tikzpicture}
preprints/A-Counterexample-to-Rysers-Covering-Conjecture-September-23-2026/build/incidence.tex ADDED
@@ -0,0 +1,707 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{A uniform incidence bound}\label{sec:incidence}
2
+
3
+ For a set $P$ of points and a set $\mathcal L$ of lines in
4
+ $\PP^2(\F_q)$, write
5
+ \begin{equation}\label{eq:inc-definition}
6
+ I(P,\mathcal L)
7
+ =\bigl|\{(p,\ell)\in P\times\mathcal L:p\in\ell\}\bigr|.
8
+ \end{equation}
9
+ Our aim is a power saving with constants independent of the field and
10
+ its characteristic. In Section~\ref{sec:linecover}, this estimate will
11
+ control intersections of a proposed line cover when no projective point
12
+ lies on many of its lines. This is the incidence input to the conclusion
13
+ that a small cover must contain almost a full pencil.
14
+
15
+ \begin{theorem}[Uniform incidence saving]\label{thm:incidence}
16
+ There exist absolute constants $\kappa\in(0,1/10)$ and $Q$ with the following
17
+ property. Suppose that $q\ge Q$ is a prime power and every proper subfield
18
+ of $\F_q$ has order at most $q^{1/3}$. If $P$ and $\mathcal L$ are sets of
19
+ projective points and projective lines over $\F_q$ satisfying
20
+ \begin{equation}\label{eq:inc-theorem-sizes}
21
+ |P|,|\mathcal L|\le q^{1+\kappa},
22
+ \end{equation}
23
+ then
24
+ \begin{equation}\label{eq:inc-theorem-bound}
25
+ I(P,\mathcal L)\le q^{3/2-\kappa}.
26
+ \end{equation}
27
+ \end{theorem}
28
+
29
+ The proof follows the incidence and sum--product strategy of
30
+ Bourgain, Katz, and Tao~\cite[Sections 3--4 and 6]{BKT2004}. Its geometric
31
+ step turns an incidence configuration with too many incidences into a
32
+ dense set of pairs whose differences and quotients range over small
33
+ sets. A graph argument then extracts one subset with both a small
34
+ difference set and a small quotient set. Finally, scalar coverings show
35
+ that such a subset cannot have size near the square root of the field
36
+ order under the proper-subfield hypothesis.
37
+
38
+ We develop the two algebraic ingredients first, then return to the
39
+ incidence configuration. The proofs include the simultaneous extraction
40
+ of additive and multiplicative control and the bounds on scalar
41
+ expressions that make the argument uniform over fields of nonprime
42
+ order.
43
+
44
+ \subsection{Finite-set estimates}
45
+
46
+ The first task is to pass from control of differences and quotients
47
+ along the edges of a dense bipartite graph to control on all pairs in
48
+ one subset. We begin with the sumset estimates needed to use the
49
+ resulting additive control.
50
+
51
+ For subsets of an abelian group, $X+Y$ and $X-Y$ denote the usual sumset
52
+ and difference set. For a nonnegative integer $j$, the notation $jY$
53
+ in this subsection means a sum of $j$ copies of $Y$, with $0Y=\{0\}$.
54
+ Later, a field element multiplying a set will always mean field scaling;
55
+ we will specify explicitly when an integer denotes an iterated sumset.
56
+
57
+ The first two estimates below are Ruzsa's triangle inequality and
58
+ covering lemma; the maximal-translates proof of the latter appears in
59
+ \cite[p.~324]{Ruzsa1999}. The multiple-sum bound is a Pl\"unnecke--Ruzsa
60
+ estimate, for which we use Petridis's minimizing-subset
61
+ proof~\cite[Proposition 2.1 and Section 3]{Petridis2012}.
62
+
63
+ \begin{lemma}[Triangle, covering, and multiple-sum estimates]
64
+ \label{inc-sumset-estimates}
65
+ Let the sets below be finite subsets of an abelian group.
66
+ \begin{enumerate}
67
+ \item If $Z$ is nonempty, then
68
+ \begin{equation}\label{eq:inc-triangle}
69
+ |X-Y|\,|Z|\le |X-Z|\,|Z-Y|.
70
+ \end{equation}
71
+ \item If $Y$ is nonempty and $|X-Y|\le M|Y|$, then $X$ is contained in
72
+ the union of at most $M$ translates of $Y-Y$.
73
+ \item If $Y$ is nonempty and $|Y-Y|\le M|Y|$, then, for all nonnegative
74
+ integers $u,v$,
75
+ \begin{equation}\label{eq:inc-multiple-sums}
76
+ |uY-vY|\le M^{u+v}|Y|.
77
+ \end{equation}
78
+ \end{enumerate}
79
+ \end{lemma}
80
+
81
+ \begin{proof}
82
+ For the triangle inequality, choose one representation $d=x_d-y_d$
83
+ for each $d\in X-Y$. The map
84
+ \[
85
+ (d,z)\longmapsto (x_d-z,z-y_d)
86
+ \]
87
+ from $(X-Y)\times Z$ into $(X-Z)\times(Z-Y)$ is injective: summing the
88
+ two coordinates recovers $d$, after which the chosen representation
89
+ recovers $z$. This proves~\eqref{eq:inc-triangle}.
90
+
91
+ For the covering statement, take a maximal set $T\subseteq X$ for
92
+ which the translates $t-Y$, $t\in T$, are pairwise disjoint. Their union
93
+ is contained in $X-Y$, so $|T|\le M$. Maximality implies that for every
94
+ $x\in X$ some $x-Y$ intersects $t-Y$ with $t\in T$, whence
95
+ $x\in t+(Y-Y)$.
96
+
97
+ For the multiple-sum bound, the minimizing-subset argument of
98
+ Petridis~\cite{Petridis2012} lets us iterate a one-step growth estimate.
99
+ Put $Q_0=-Y$ and choose a nonempty
100
+ $W\subseteq Y$ minimizing
101
+ \[
102
+ \mu=\frac{|W+Q_0|}{|W|}.
103
+ \]
104
+ Then $\mu\le M$, and every $W'\subseteq W$, including the empty set,
105
+ satisfies $|W'+Q_0|\ge\mu|W'|$. We claim that for every finite set $E_0$,
106
+ \begin{equation}\label{eq:inc-petridis-growth}
107
+ |W+Q_0+E_0|\le\mu|W+E_0|.
108
+ \end{equation}
109
+ The assertion is immediate if $E_0$ is empty. Otherwise order its
110
+ elements as $e_1,\ldots,e_k$. When the translate $W+e_i$ is added to
111
+ the preceding translates, let
112
+ \[
113
+ W_i'=\{w\in W:w+e_i\in\bigcup_{j<i}(W+e_j)\}.
114
+ \]
115
+ It contributes exactly $|W|-|W_i'|$ new elements. Moreover,
116
+ $W_i'+Q_0+e_i$ is contained in the union of the preceding enlarged
117
+ translates $W+Q_0+e_j$. Thus the contribution of $W+Q_0+e_i$ is at most
118
+ \[
119
+ |W+Q_0|-|W_i'+Q_0|
120
+ \le\mu\bigl(|W|-|W_i'|\bigr).
121
+ \]
122
+ Summing proves~\eqref{eq:inc-petridis-growth}. Iterating this estimate
123
+ gives $|W+jQ_0|\le\mu^j|W|$ for every nonnegative integer $j$.
124
+ We now remove the auxiliary set $W$ by applying
125
+ \eqref{eq:inc-triangle} to $uQ_0,vQ_0$ with intermediate set $-W$:
126
+ \[
127
+ |uQ_0-vQ_0|\,|W|
128
+ \le |W+uQ_0|\,|W+vQ_0|
129
+ \le\mu^{u+v}|W|^2.
130
+ \]
131
+ Negation preserves cardinality, so $|uQ_0-vQ_0|=|uY-vY|$. Since
132
+ $|W|\le|Y|$ and $\mu\le M$, this is~\eqref{eq:inc-multiple-sums}.
133
+ \end{proof}
134
+
135
+ We next carry out the extraction from a dense graph. The argument uses
136
+ the common-neighborhood method in Gowers's quantitative refinement
137
+ \cite[Section 4, Lemma 11 and Proposition 12]{Gowers1998} of the
138
+ Balog--Szemer\'edi theorem~\cite{BalogSzemeredi1994}; see also
139
+ \cite[Section 5, Lemmas 5.1--5.2]{FoxSudakov2011}. The point is to use the same walks
140
+ for both additive and multiplicative edge labels. We can therefore
141
+ obtain both bounds on one subset, which is what the subsequent
142
+ subfield argument requires. In the geometric application, the edge
143
+ labels will come from the four pencils through four chosen points.
144
+
145
+ \begin{lemma}[Simultaneous difference and quotient extraction]
146
+ \label{inc-simultaneous-extraction}
147
+ Let $F$ be a field, let $A,B\subseteq F^*$ be finite, and let
148
+ $G\subseteq A\times B$. Define
149
+ \[
150
+ D=\{a-b:(a,b)\in G\},\qquad
151
+ J=\{a/b:(a,b)\in G\}.
152
+ \]
153
+ Suppose that, for real numbers $n>0$ and $V\ge2$,
154
+ \begin{equation}\label{eq:inc-graph-hypotheses}
155
+ |A|,|B|,|D|,|J|\le Vn,
156
+ \qquad |G|\ge n^2/V.
157
+ \end{equation}
158
+ Then there is $S\subseteq A$ such that
159
+ \begin{equation}\label{eq:inc-extracted-size}
160
+ \frac{3n}{8V^2}\le |S|\le Vn
161
+ \end{equation}
162
+ and
163
+ \begin{equation}\label{eq:inc-extracted-expansion}
164
+ |S-S|,|S/S|\le 2^{20}V^{22}n.
165
+ \end{equation}
166
+ Here $S/S=\{a/a':a,a'\in S\}$.
167
+ \end{lemma}
168
+
169
+ \begin{proof}
170
+ We first find a large set of vertices such that every ordered pair
171
+ is joined by many walks of length four. Counting the possible edge
172
+ labels of these walks will then bound both differences and quotients
173
+ of the endpoints.
174
+
175
+ Regard $G$ as a bipartite graph, and put
176
+ $\tau=(512V^8)^{-1}$. Call an ordered pair $(a,a_2)\in A^2$ bad if
177
+ it has fewer than $\tau n$ common neighbors in $B$. To find a
178
+ neighborhood with few bad pairs, first note that vertices of $B$
179
+ with fewer than $n/(2V^2)$ neighbors account for at most
180
+ $|B|n/(2V^2)\le n^2/(2V)$ edges. Since every vertex of $B$ has at
181
+ most $Vn$ neighbors, the set of vertices with at least $n/(2V^2)$
182
+ neighbors has size at least $n/(2V^2)$.
183
+
184
+ Summed over all $b\in B$, the number of bad ordered pairs in the
185
+ neighborhood of $b$ is at most
186
+ \[
187
+ |A|^2\tau n\le V^2\tau n^3.
188
+ \]
189
+ Averaging over the large neighborhoods just identified, one obtains
190
+ a neighborhood $A_0$ of size at least $n/(2V^2)$ in which the number
191
+ of bad ordered pairs is at most
192
+ \[
193
+ 2V^4\tau n^2=\frac{n^2}{256V^4}
194
+ \le \frac{|A_0|^2}{64}
195
+ \le \frac{|A_0|^2}{16}.
196
+ \]
197
+ Let $S$ consist of those $a\in A_0$ having at most $|A_0|/4$ bad
198
+ partners in $A_0$. At most $|A_0|/4$ elements are discarded, so
199
+ $|S|\ge3|A_0|/4$, proving~\eqref{eq:inc-extracted-size}.
200
+
201
+ The choice of $S$ ensures that, for every $a,a'\in S$, at least
202
+ $|A_0|/2$ elements $a_2\in A_0$ form nonbad pairs with both endpoints.
203
+ Each such $a_2$ gives at least $(\tau n)^2$
204
+ ordered walks
205
+ \[
206
+ a,b_1,a_2,b_2,a'
207
+ \]
208
+ whose four edges belong to $G$. Repeated vertices are allowed.
209
+ Consequently each ordered endpoint pair in $S^2$ has at least
210
+ \begin{equation}\label{eq:inc-walk-count}
211
+ \frac{|A_0|}{2}(\tau n)^2
212
+ \ge\frac{n^3}{2^{20}V^{18}}
213
+ \end{equation}
214
+ such walks. This lower bound now converts the limited number of edge
215
+ labels into a bound on endpoint differences.
216
+
217
+ For one of these walks, write its edge differences, always taking
218
+ the $A$ coordinate minus the $B$ coordinate, as
219
+ \[
220
+ d_1=a-b_1,\quad d_2=a_2-b_1,\quad
221
+ d_3=a_2-b_2,\quad d_4=a'-b_2.
222
+ \]
223
+ They satisfy $a-a'=d_1-d_2+d_3-d_4$. For a fixed endpoint pair,
224
+ the four differences determine the walk uniquely: starting from $a$,
225
+ one recovers successively $b_1,a_2,b_2,a'$. Choose one ordered
226
+ endpoint pair for each element of $S-S$. The resulting collections
227
+ of difference quadruples are disjoint for different differences,
228
+ because their alternating sums differ. Counting in $D^4$ and using
229
+ \eqref{eq:inc-walk-count} gives
230
+ \[
231
+ |S-S|\le
232
+ \frac{|D|^4}{n^3/(2^{20}V^{18})}
233
+ \le 2^{20}V^{22}n.
234
+ \]
235
+
236
+ The same walks give the quotient bound on the same set $S$. Put
237
+ \[
238
+ j_1=a/b_1,\quad j_2=a_2/b_1,\quad
239
+ j_3=a_2/b_2,\quad j_4=a'/b_2.
240
+ \]
241
+ All are nonzero, and $a/a'=j_1j_3/(j_2j_4)$. From a fixed initial
242
+ $a$ and these four quotients one recovers
243
+ $b_1=a/j_1$, $a_2=j_2b_1$, $b_2=a_2/j_3$, and $a'=j_4b_2$.
244
+ Choosing one endpoint pair for each element of $S/S$ and counting
245
+ in $J^4$ therefore proves the other bound in
246
+ \eqref{eq:inc-extracted-expansion}.
247
+ \end{proof}
248
+
249
+ \subsection{Bounded scalar expressions and subfields}
250
+
251
+ We now turn to the algebraic obstruction: a set near the square-root
252
+ field scale cannot have both the small difference set and the small
253
+ quotient set supplied by the extraction lemma. The first step is to
254
+ bound sums involving scalars formed using a bounded number of field
255
+ operations. We use the scalar-covering method of Bourgain, Katz, and
256
+ Tao~\cite[Lemma 3.2 and Proposition 3.3]{BKT2004}, keeping the dependence
257
+ on the number of operations explicit.
258
+
259
+ An expression in a set $E\subseteq F$ is built from members of
260
+ $E\cup\{0,1\}$ using binary addition, subtraction, and multiplication,
261
+ and unary negation and inversion. Each of these operations counts
262
+ as one operation. Inversion is allowed only when its argument is
263
+ nonzero.
264
+
265
+ \begin{lemma}[Uniform scalar coverings]\label{inc-scalar-coverings}
266
+ Let $B$ be a nonempty finite subset of a field $F$, let $E\subseteq B$,
267
+ and let $K\ge2$. Suppose that
268
+ \begin{equation}\label{eq:inc-scalar-hypotheses}
269
+ |B-B|\le K|B|,
270
+ \qquad |B-eB|\le 2K^3|B|\quad(e\in E).
271
+ \end{equation}
272
+ Define
273
+ \begin{equation}\label{eq:inc-scalar-exponents}
274
+ C_0=4,\qquad C_{m+1}=3C_m+5,
275
+ \qquad\text{so that }C_m=\frac{13\cdot3^m-5}{2}.
276
+ \end{equation}
277
+ If $\lambda\in F$ has an expression in $E$ using at most $m$
278
+ operations, then $\lambda B$ is contained in at most $K^{C_m}$
279
+ translates of $B-B$. In particular,
280
+ \begin{equation}\label{eq:inc-scalar-sum-bound}
281
+ |E+\lambda E|\le |B+\lambda B|
282
+ \le K^{C_m+3}|B|.
283
+ \end{equation}
284
+ These bounds are uniform over all such expressions and all choices
285
+ of their entries from $E$.
286
+ \end{lemma}
287
+
288
+ \begin{proof}
289
+ Put $H=B-B$, so $H=-H$ and $0\in H$. In the remainder of this proof,
290
+ integer multiples of $B$ or $H$ inside sumsets denote iterated sums.
291
+ We prove the covering assertion by induction on expression length.
292
+ To combine coverings at an induction step, we will need a fixed
293
+ covering of $2H$ by translates of $H$. By
294
+ Lemma~\ref{inc-sumset-estimates},
295
+ \[
296
+ |2H-B|=|2B-3B|\le K^5|B|.
297
+ \]
298
+ The covering statement of that lemma consequently supplies a set
299
+ $T_*\subseteq F$ with $|T_*|\le K^5$ such that
300
+ \begin{equation}\label{eq:inc-two-differences-cover}
301
+ 2H\subseteq T_*+H.
302
+ \end{equation}
303
+
304
+ Every $e\in E$ has a covering $eB\subseteq T_e+H$ with
305
+ $|T_e|\le2K^3\le K^4$, by
306
+ \eqref{eq:inc-scalar-hypotheses} and the covering lemma.
307
+ The scalars $0$ and $1$ also have coverings by one translate of $H$:
308
+ use $\{0\}\subseteq H$ and $B\subseteq b_0+H$ for any $b_0\in B$.
309
+ This proves the case $m=0$.
310
+
311
+ We now check how the number of translates changes under each allowed
312
+ operation. Suppose that
313
+ \[
314
+ \lambda B\subseteq T+H,\qquad
315
+ \mu B\subseteq U+H,\qquad
316
+ |T|\le K^a,\quad |U|\le K^b.
317
+ \]
318
+ Negation replaces $T$ by $-T$. For addition and subtraction,
319
+ \[
320
+ (\lambda\pm\mu)B
321
+ \subseteq \lambda B\pm\mu B
322
+ \subseteq T\pm U+2H
323
+ \subseteq T\pm U+T_*+H,
324
+ \]
325
+ so the number of translates is at most $K^{a+b+5}$. For a product,
326
+ \[
327
+ \lambda\mu B
328
+ \subseteq \lambda U+\lambda H
329
+ =\lambda U+(\lambda B-\lambda B)
330
+ \subseteq\lambda U+T-T+T_*+H.
331
+ \]
332
+ This uses at most $K^{b+2a+5}$ translates and is valid even if
333
+ $\lambda=0$. Finally, if $\lambda\ne0$, then
334
+ \[
335
+ |\lambda B-B|
336
+ \le |T|\,|H-B|
337
+ =|T|\,|B-2B|
338
+ \le K^{a+3}|B|.
339
+ \]
340
+ Scaling by $\lambda^{-1}$ and then negating gives
341
+ $|\lambda^{-1}B-B|\le K^{a+3}|B|$. The covering lemma now covers
342
+ $\lambda^{-1}B$ by at most $K^{a+3}$ translates of $H$.
343
+
344
+ These bounds give the claimed uniform induction: in an expression
345
+ with at most $m+1$ operations, each immediate subexpression has at
346
+ most $m$ operations, so every resulting covering uses at most
347
+ $K^{3C_m+5}$ translates. This proves the covering assertion
348
+ with~\eqref{eq:inc-scalar-exponents}.
349
+
350
+ To deduce the sumset bound from the covering, let
351
+ $\lambda B\subseteq T+H$ be the covering just obtained. Then
352
+ \[
353
+ |B+\lambda B|
354
+ \le |T|\,|B+H|
355
+ =|T|\,|2B-B|
356
+ \le K^{C_m+3}|B|,
357
+ \]
358
+ again by Lemma~\ref{inc-sumset-estimates}. Since $E\subseteq B$,
359
+ this also bounds $|E+\lambda E|$.
360
+ \end{proof}
361
+
362
+ When working along a sequence $q\to\infty$, a positive quantity
363
+ $K=q^{o(1)}$ means that $\log K/\log q\to0$. Likewise,
364
+ $|S|=q^{1/2+o(1)}$ means that $\log|S|/\log q\to1/2$.
365
+ In particular, every fixed power of a subpower factor is still a
366
+ subpower factor. This is why a uniform bound for expressions of
367
+ fixed length suffices for the next lemma.
368
+
369
+ \begin{lemma}[Exclusion of an intermediate approximate subfield]
370
+ \label{inc-no-approximate-subfield}
371
+ There is no sequence of prime powers $q\to\infty$, each satisfying
372
+ the proper-subfield hypothesis of Theorem~\ref{thm:incidence}, together
373
+ with sets $S\subseteq\F_q^*$ and numbers $K\ge2$ such that
374
+ \begin{equation}\label{eq:inc-approximate-subfield-hypotheses}
375
+ |S|=q^{1/2+o(1)},\qquad K=q^{o(1)},\qquad
376
+ |S-S|,|S/S|\le K|S|.
377
+ \end{equation}
378
+ \end{lemma}
379
+
380
+ \begin{proof}
381
+ Suppose that such a sequence exists. We first use multiplicative
382
+ overlaps to obtain sets satisfying the scalar-covering hypotheses.
383
+ Ratios of differences in a large subset will then form a subfield.
384
+ The proper-subfield hypothesis will force that subfield to be the
385
+ whole field, where averaging will contradict the scalar-covering
386
+ bound.
387
+
388
+ \paragraph{Extracting scalar-covering hypotheses.}
389
+ Put $s=|S|$. The $s$ sets
390
+ $S/a$, $a\in S$, each have size $s$, and their union is contained
391
+ in $S/S$. Cauchy--Schwarz gives
392
+ \begin{equation}\label{eq:inc-multiplicative-overlaps}
393
+ \sum_{a,b\in S}|S/a\cap S/b|
394
+ \ge\frac{s^4}{|S/S|}\ge\frac{s^3}{K}.
395
+ \end{equation}
396
+ Thus some $b\in S$ satisfies
397
+ $\sum_{a\in S}|S/a\cap S/b|\ge s^2/K$.
398
+ Since every summand is at most $s$, at least $s/(2K)$ values
399
+ $a\in S$ have $|S/a\cap S/b|\ge s/(2K)$: otherwise the sum of
400
+ the large summands would be less than $s^2/(2K)$ and that of all
401
+ the other summands at most $s^2/(2K)$.
402
+
403
+ Let $E$ be the set of $e=a/b$ for these values of $a$, and put
404
+ $B=S/b$. Then
405
+ \begin{equation}\label{eq:inc-overlap-subset}
406
+ E\subseteq B,\qquad |B|=s,\qquad
407
+ |E|\ge\frac{s}{2K},\qquad
408
+ |S\cap eS|\ge\frac{s}{2K}\quad(e\in E).
409
+ \end{equation}
410
+ The last inequality follows by multiplying $S/a\cap S/b$ by $a$.
411
+ For $Z=S\cap eS$, the triangle inequality and the containments
412
+ $Z\subseteq S,eS$ imply
413
+ \[
414
+ |S-eS|
415
+ \le\frac{|S-Z|\,|Z-eS|}{|Z|}
416
+ \le\frac{(Ks)^2}{s/(2K)}=2K^3s.
417
+ \]
418
+ After scaling by $1/b$, we have
419
+ \[
420
+ |B-B|\le Ks,\qquad |B-eB|\le2K^3s\quad(e\in E).
421
+ \]
422
+ Thus Lemma~\ref{inc-scalar-coverings} applies to $B$ and $E$.
423
+ We have obtained uniform control for every scalar expressible using
424
+ a bounded number of operations on elements of $E$.
425
+
426
+ \paragraph{Ratios of differences form a subfield.}
427
+ Write $t=|E|$. By~\eqref{eq:inc-overlap-subset} and
428
+ \eqref{eq:inc-approximate-subfield-hypotheses},
429
+ $t=q^{1/2+o(1)}$. In particular, $t\ge2$ for all sufficiently
430
+ large fields in the sequence. Define
431
+ \begin{equation}\label{eq:inc-ratio-set}
432
+ R_0=\left\{\frac{x-x'}{y-y'}:
433
+ x,x',y,y'\in E,\ y\ne y'\right\}.
434
+ \end{equation}
435
+ To prove closure under addition and multiplication, we apply the
436
+ scalar-covering bound to the result of either operation.
437
+ Every member of $R_0$ has an expression in $E$ with at most four
438
+ operations. Consequently, for $r,r'\in R_0$, each of $r+r'$ and
439
+ $rr'$ has an expression with at most nine operations. For either
440
+ candidate $\lambda$, Lemma~\ref{inc-scalar-coverings} gives
441
+ \[
442
+ |E+\lambda E|\le K^{C_9+3}s<t^2
443
+ \]
444
+ for all sufficiently large $q$, uniformly over $r,r'$.
445
+ Indeed, the ratio of this upper bound to $t^2$ is at most
446
+ $4K^{C_9+5}/s$, which tends to zero. Therefore the map
447
+ $(x,y)\mapsto x+\lambda y$ from $E^2$ is not injective. A collision
448
+ between distinct pairs satisfies $y\ne y'$, since otherwise also
449
+ $x=x'$, and gives
450
+ \[
451
+ \lambda=\frac{x'-x}{y-y'}\in R_0.
452
+ \]
453
+ It follows that $R_0$ is closed under addition and multiplication.
454
+ It contains $0$ and $1$ and, directly from its definition, is closed
455
+ under negation and reciprocals of nonzero elements. Thus $R_0$ is a
456
+ subfield of $\F_q$.
457
+
458
+ The size of $E$ now prevents this subfield from being proper.
459
+ Choose distinct $e_0,e_1\in E$. The map
460
+ \[
461
+ e\longmapsto\frac{e-e_0}{e_1-e_0}
462
+ \]
463
+ injects $E$ into $R_0$, so $|R_0|\ge t>q^{1/3}$ for large $q$.
464
+ The proper-subfield hypothesis forces $R_0=\F_q$.
465
+
466
+ \paragraph{A scalar with a large sumset.}
467
+ Every field element consequently has a four-operation representation
468
+ using elements of $E$. The scalar-covering estimate therefore bounds
469
+ $|E+\lambda E|$ for every scalar. To reach a contradiction, we average
470
+ over the field and find a scalar for which this sumset is too large.
471
+
472
+ For $\lambda\in\F_q$, let $N_\lambda$ be the number of ordered
473
+ quadruples $(x,y,x',y')\in E^4$ satisfying
474
+ $x+\lambda y=x'+\lambda y'$. There are $t^2$ identical pairs,
475
+ which give a collision for every $\lambda$. If $y\ne y'$, exactly
476
+ one value of $\lambda$ gives a collision; if $y=y'$ but $x\ne x'$,
477
+ none does. Hence
478
+ \begin{equation}\label{eq:inc-average-collisions}
479
+ \frac1q\sum_{\lambda\in\F_q}N_\lambda
480
+ =t^2+\frac{t^4-t^3}{q}
481
+ \le t^2+\frac{t^4}{q}.
482
+ \end{equation}
483
+ For some $\lambda$, Cauchy--Schwarz applied to the fibers of
484
+ $(x,y)\mapsto x+\lambda y$ therefore yields
485
+ \begin{equation}\label{eq:inc-large-dilate-sum}
486
+ |E+\lambda E|
487
+ \ge\frac{t^4}{t^2+t^4/q}
488
+ \ge\frac12\min(t^2,q)
489
+ =q^{1-o(1)}.
490
+ \end{equation}
491
+ But $R_0=\F_q$, so this particular $\lambda$ itself has a
492
+ four-operation representation in~\eqref{eq:inc-ratio-set}.
493
+ Lemma~\ref{inc-scalar-coverings} bounds its sumset by
494
+ $K^{C_4+3}s=q^{1/2+o(1)}$, contradicting
495
+ \eqref{eq:inc-large-dilate-sum}. The expression length here remains
496
+ bounded; no iteration of field generation is being used.
497
+ \end{proof}
498
+
499
+ \Needspace{10\baselineskip}
500
+ \subsection{Proof of the incidence theorem}
501
+
502
+ The algebraic ingredients are now in place. It remains to obtain the
503
+ hypotheses of Lemma~\ref{inc-simultaneous-extraction} from a configuration
504
+ with too many incidences. We use the projective-coordinate reduction
505
+ in the incidence strategy of Bourgain, Katz, and
506
+ Tao~\cite[Section 6]{BKT2004}: after controlling degrees, we choose four
507
+ points whose pencils encode the two coordinates, their difference,
508
+ and their quotient.
509
+
510
+ \begin{proof}[Proof of Theorem~\ref{thm:incidence}]
511
+ We argue by contradiction, allowing all quantitative losses to be
512
+ subpower factors along a sequence of fields. Suppose the theorem is
513
+ false. For a sequence of positive exponents
514
+ $\kappa_j\to0$ in $(0,1/10)$, choose admissible counterexamples with
515
+ $q_j\to\infty$. Such choices are possible because the failure of
516
+ the theorem says that for each fixed exponent there are arbitrarily
517
+ large counterexamples. Along this sequence, put
518
+ $U=\max(2,q_j^{\kappa_j})$ and suppress the index $j$. We have
519
+ \begin{equation}\label{eq:inc-counterexample-sequence}
520
+ |P|,|\mathcal L|\le Uq,\qquad
521
+ I(P,\mathcal L)\ge\frac{q^{3/2}}{U},\qquad
522
+ U\ge2,\qquad U=q^{o(1)}.
523
+ \end{equation}
524
+ All bounds below use absolute constants. Every assertion made for
525
+ sufficiently large $q$ is along this sequence. Our goal is to construct
526
+ from these counterexamples sets of the size and small-expansion form
527
+ excluded by Lemma~\ref{inc-no-approximate-subfield}.
528
+
529
+ \paragraph{Pruning the incidence graph.}
530
+ We first retain many incidences while putting both an upper and a
531
+ lower bound on every remaining degree. Consider the bipartite graph
532
+ on $P$ and $\mathcal L$ whose edges are incidences. If $d(v)$ denotes a degree on either side, then counting
533
+ ordered pairs on the opposite side and using the unique join of two
534
+ distinct projective points, or the unique intersection of two
535
+ distinct projective lines, gives
536
+ \begin{equation}\label{eq:inc-degree-squares}
537
+ \sum_v d(v)^2\le2U^2q^2
538
+ \quad\text{on each side}.
539
+ \end{equation}
540
+ Here $\sum_vd(v)(d(v)-1)\le U^2q^2$, and
541
+ $\sum_vd(v)=I(P,\mathcal L)\le U^2q^2$.
542
+
543
+ Set
544
+ \begin{equation}\label{eq:inc-degree-cutoffs}
545
+ H=16U^3q^{1/2},\qquad d=\frac{q^{1/2}}{8U^2}.
546
+ \end{equation}
547
+ Delete every vertex whose initial degree exceeds $H$. By
548
+ \eqref{eq:inc-degree-squares}, the total number of incidences lost,
549
+ counting both sides, is at most
550
+ \[
551
+ \frac{4U^2q^2}{H}=\frac{q^{3/2}}{4U}.
552
+ \]
553
+ Next, iteratively delete vertices whose current degree is less than
554
+ $d$. Each of the at most $2Uq$ original vertices is deleted at most
555
+ once, so this stage loses at most
556
+ $2Uq\,d=q^{3/2}/(4U)$ incidences. Denote the surviving sets again by
557
+ $P,\mathcal L$. They satisfy
558
+ \begin{equation}\label{eq:inc-pruned-bounds}
559
+ I(P,\mathcal L)\ge\frac{q^{3/2}}{2U},\qquad
560
+ \frac{q}{32U^4}\le |P|,|\mathcal L|\le Uq,
561
+ \qquad d\le d(v)\le H.
562
+ \end{equation}
563
+ The size lower bounds follow by dividing the surviving incidence
564
+ count by the maximum degree $H$.
565
+
566
+ The pruning also controls the intersection of $P$ with
567
+ \emph{every} projective line, including lines not in $\mathcal L$.
568
+ We will need this stronger form of control when discarding points
569
+ on a few lines chosen later. Fix a projective line $\ell$. Each point
570
+ of $P\cap\ell$ is incident with at least $d-1$ lines of $\mathcal L$ different from $\ell$.
571
+ These lines are distinct for different points of $P\cap\ell$.
572
+ Since $d\to\infty$, for large $q$ we obtain
573
+ \begin{equation}\label{eq:inc-all-line-cap}
574
+ |P\cap\ell|
575
+ \le\frac{|\mathcal L|}{d-1}
576
+ \le16U^3q^{1/2}=H
577
+ \qquad\text{for every projective line }\ell.
578
+ \end{equation}
579
+
580
+ \paragraph{Four anchors with many common witnesses.}
581
+ We seek four points, three collinear and the fourth off their line,
582
+ together with many points joined to each of them by lines of
583
+ $\mathcal L$. We obtain the four points by first counting such
584
+ configurations around each possible common point and then averaging.
585
+
586
+ For $x\in P$, let $N(x)$ consist of the points in $P\setminus\{x\}$
587
+ joined to $x$ by a line of $\mathcal L$. Distinct lines through $x$
588
+ have disjoint point sets away from $x$, so
589
+ \begin{equation}\label{eq:inc-neighborhood-size}
590
+ |N(x)|\ge d(d-1)\ge\frac{q}{128U^4}
591
+ \end{equation}
592
+ for large $q$. Put $t_\ell=|N(x)\cap\ell|$. Summing degrees of the
593
+ points of $N(x)$ gives
594
+ \[
595
+ \sum_{\ell\in\mathcal L}t_\ell
596
+ \ge d|N(x)|\ge\frac{q^{3/2}}{1024U^6}.
597
+ \]
598
+ Lines with $t_\ell\le2$ contribute at most $2Uq$. Because $U=q^{o(1)}$,
599
+ for sufficiently large $q$ this is at most half of the displayed
600
+ lower bound. Consequently
601
+ \[
602
+ \sum_{\ell:t_\ell\ge3}t_\ell
603
+ \ge\frac{q^{3/2}}{2048U^6}.
604
+ \]
605
+ For every integer $t\ge3$, one has
606
+ $t(t-1)(t-2)\ge(2/9)t^3$. H\"older's inequality therefore shows
607
+ that the number of ordered triples of distinct points of $N(x)$
608
+ lying on a line of $\mathcal L$ is at least
609
+ \begin{equation}\label{eq:inc-collinear-triples}
610
+ \begin{split}
611
+ \sum_{\ell\in\mathcal L}t_\ell(t_\ell-1)(t_\ell-2)
612
+ &\ge\frac{2}{9|\mathcal L|^2}
613
+ \left(\sum_{\ell:t_\ell\ge3}t_\ell\right)^3\\
614
+ &\ge\frac{q^{5/2}}{9\cdot2^{32}U^{20}}.
615
+ \end{split}
616
+ \end{equation}
617
+ By~\eqref{eq:inc-all-line-cap} and
618
+ \eqref{eq:inc-neighborhood-size}, each such triple admits at least
619
+ \[
620
+ \frac{q}{128U^4}-H\ge\frac{q}{256U^4}
621
+ \]
622
+ choices of a fourth point in $N(x)$ outside its line, once $q$ is
623
+ large enough. Summing over $x$ and using
624
+ \eqref{eq:inc-pruned-bounds}, we obtain at least
625
+ \begin{equation}\label{eq:inc-witness-quadruple-count}
626
+ \frac{q^{9/2}}{9\cdot2^{45}U^{28}}
627
+ \end{equation}
628
+ ordered choices $(x,p_1,p_2,p_3,p_4)$ with $p_1,p_2,p_3$ distinct
629
+ and collinear on a line of $\mathcal L$, with $p_4$ outside that
630
+ line, and with all four $p_i$ in $N(x)$.
631
+
632
+ We now reverse the count to fix the four anchor points while retaining
633
+ many choices of the common point $x$. The number of possible ordered
634
+ quadruples $(p_1,p_2,p_3,p_4)$ in this count is at most
635
+ \begin{equation}\label{eq:inc-quadruple-upper-bound}
636
+ |\mathcal L|H^3|P|
637
+ \le2^{12}U^{11}q^{7/2}.
638
+ \end{equation}
639
+ Some quadruple thus has at least
640
+ \begin{equation}\label{eq:inc-common-witnesses}
641
+ c_0\frac{q}{U^{39}}
642
+ \quad\text{witnesses }x,\qquad
643
+ c_0=\frac1{9\cdot2^{57}}.
644
+ \end{equation}
645
+ Discard the witnesses on the common line of $p_1,p_2,p_3$ and on
646
+ the joins of $p_1,p_4$ and of $p_2,p_4$. The cap
647
+ \eqref{eq:inc-all-line-cap} discards at most $3H$ witnesses.
648
+ Since $U=q^{o(1)}$, this is eventually less than
649
+ $c_0q/(2U^{39})$. At least that many witnesses remain. Their joins
650
+ to the four anchors will supply the graph and the four small sets
651
+ required by Lemma~\ref{inc-simultaneous-extraction}.
652
+
653
+ \paragraph{The four pencils as coordinates.}
654
+ Choose projective coordinates in which
655
+ \[
656
+ p_1=(1:0:0),\qquad p_2=(0:1:0),\qquad
657
+ p_3=(1:1:0),\qquad p_4=(0:0:1).
658
+ \]
659
+ This is possible over $\F_q$: representatives of $p_1,p_2$ span
660
+ their line, the representative of the distinct third point has
661
+ both coefficients nonzero and permits rescaling of the first two,
662
+ and a representative of $p_4$ completes a basis. The discarded
663
+ lines are precisely the coordinate line at infinity and the two
664
+ coordinate axes through $p_4$. Hence every remaining witness has
665
+ coordinates $(a:b:1)$ with $a,b\ne0$.
666
+
667
+ Let $G$ be the set of these pairs $(a,b)$, and let $A,B$ be its
668
+ coordinate projections. Define $D$ and $J$ from $G$ as in
669
+ Lemma~\ref{inc-simultaneous-extraction}. The chosen coordinates make
670
+ the roles of the four pencils explicit: for a witness $(a:b:1)$,
671
+ the joins to $p_2,p_1,p_3,p_4$, respectively, have equations
672
+ \[
673
+ X=aZ,\qquad Y=bZ,\qquad
674
+ X-Y=(a-b)Z,\qquad X=(a/b)Y.
675
+ \]
676
+ Each join is a member of $\mathcal L$, by the witness property.
677
+ Each anchor belongs to $P$ and has degree at most $H$.
678
+ Distinct values of the corresponding parameter give distinct
679
+ lines in its pencil. Thus
680
+ \[
681
+ |A|,|B|,|D|,|J|\le H,
682
+ \qquad |G|\ge\frac{c_0q}{2U^{39}}.
683
+ \]
684
+ With
685
+ \begin{equation}\label{eq:inc-graph-parameters}
686
+ n=q^{1/2},\qquad V=\frac{2}{c_0}U^{39},
687
+ \end{equation}
688
+ we have $V\ge2$, $V=q^{o(1)}$, and all the hypotheses
689
+ \eqref{eq:inc-graph-hypotheses} hold.
690
+
691
+ The incidence configuration now meets the extraction hypotheses.
692
+ Lemma~\ref{inc-simultaneous-extraction} gives
693
+ $S\subseteq\F_q^*$ satisfying
694
+ \[
695
+ \frac{3q^{1/2}}{8V^2}\le |S|\le Vq^{1/2},\qquad
696
+ |S-S|,|S/S|\le2^{20}V^{22}q^{1/2}.
697
+ \]
698
+ In particular $|S|=q^{1/2+o(1)}$, and, on setting
699
+ $K=2^{23}V^{24}$, we have $K\ge2$, $K=q^{o(1)}$, and
700
+ $|S-S|,|S/S|\le K|S|$. This contradicts
701
+ Lemma~\ref{inc-no-approximate-subfield}.
702
+
703
+ We have excluded every sequence of counterexamples of the form
704
+ \eqref{eq:inc-counterexample-sequence}. The negation of the theorem
705
+ would have produced such a sequence, so some absolute
706
+ $\kappa\in(0,1/10)$ and $Q$ satisfy the stated conclusion.
707
+ \end{proof}
preprints/A-Counterexample-to-Rysers-Covering-Conjecture-September-23-2026/build/linecover.tex ADDED
@@ -0,0 +1,447 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Line covers after random deletions}\label{sec:linecover}
2
+
3
+ We regard the affine plane $\F_q^2$ as a subset of its projective
4
+ completion $\PP^2(\F_q)$. Thus a pencil with centre at infinity is a
5
+ parallel class of affine lines. The purpose of this section is to show
6
+ that a set of at most $q$ lines covering almost all survivors of a
7
+ suitable random deletion process must contain almost a full pencil.
8
+ The deletions within a single trial may be dependent; independence is
9
+ required only between trials.
10
+
11
+ Classical covering results for finite planes are closely related by
12
+ duality to blocking sets. Jamison and Brouwer--Schrijver established the
13
+ affine blocking-set lower bound $2q-1$~\cite{Jamison1977,BrouwerSchrijver1978},
14
+ and Blokhuis, Brouwer, and Sz\H{o}nyi studied partial projective covers
15
+ and bounds depending on their uncovered points
16
+ \cite[Section 1.1, Proposition 1.5]{BBS2010}. Here the covered set instead consists of the
17
+ positive-density survivors of structured random deletions. We prove the
18
+ pencil statement needed in this setting directly.
19
+
20
+ There are two different concentration tasks. The total number of
21
+ surviving points and the number on a fixed line have bounded changes
22
+ under one trial; for these we use the elementary estimates
23
+ in~\cite[Lemmas~A.2--A.3]{OpenAI2026Balanced}. The more delicate task
24
+ is to retain many intersections of a short list of lines, simultaneously
25
+ for every such list. A deletion trial rarely hits this small set, and
26
+ we must use that rarity in the variance estimate. We prove the needed
27
+ Bernstein-type martingale bound here, following the method of
28
+ Freedman~\cite[Theorem (1.6) and Proposition (2.1)]{Freedman1975}.
29
+
30
+ \begin{lemma}[Martingale concentration]\label{lem:martingale}
31
+ Let $Z_i$, $1\leq i\leq n$, be martingale differences for a filtration
32
+ $(\mathcal A_i)_{i=0}^n$. Suppose that $M,V>0$ and deterministic numbers
33
+ $v_i\geq0$ satisfy, almost surely,
34
+ \[
35
+ |Z_i|\leq M,\qquad
36
+ \E(Z_i^2\mid\mathcal A_{i-1})\leq v_i,\qquad
37
+ \sum_{i=1}^n v_i\leq V.
38
+ \]
39
+ Then, for every $u>0$,
40
+ \begin{equation}\label{eq:lc-martingale}
41
+ \Pr\left(\left|\sum_{i=1}^n Z_i\right|\geq u\right)
42
+ \leq 2\exp\left[-\frac14
43
+ \min\left\{\frac{u^2}{V},\frac{u}{M}\right\}\right].
44
+ \end{equation}
45
+ \end{lemma}
46
+
47
+ \begin{proof}
48
+ For $|z|\leq1$ we have $e^z\leq1+z+z^2$. Consequently, if
49
+ $|\theta|\leq M^{-1}$, the conditional mean-zero property gives
50
+ \[
51
+ \E(e^{\theta Z_i}\mid\mathcal A_{i-1})
52
+ \leq 1+\theta^2v_i\leq e^{\theta^2v_i}.
53
+ \]
54
+ Iteration and Markov's inequality bound the upper tail by
55
+ $\exp(\theta^2V-\theta u)$ for $0<\theta\leq M^{-1}$.
56
+ Take $\theta=\min\{u/(2V),1/M\}$. If $u\leq2V/M$, the exponent is
57
+ $-u^2/(4V)$; otherwise it is at most $-u/(2M)$.
58
+ Applying the same argument to $-Z_i$ proves
59
+ \eqref{eq:lc-martingale}.
60
+
61
+ \end{proof}
62
+
63
+ \begin{lemma}[Line covers after random deletions]\label{lem:linecover}
64
+ Let $q\to\infty$ through prime powers for which every proper subfield
65
+ of $\F_q$ has order at most $q^{1/3}$. Fix a positive integer $D$ and
66
+ constants $\delta>0$ and $0<\rho<1$. For each $q$, let $\mathcal F$ be a
67
+ family of at most $Dq^D$ subsets of $\F_q^2$, called shapes, such that
68
+ \begin{enumerate}
69
+ \item every $F\in\mathcal F$ has at most $Dq$ points;
70
+ \item for every $F\in\mathcal F$ and affine line $\ell$, either
71
+ $F=\ell$ or $|F\cap\ell|\leq D$.
72
+ \end{enumerate}
73
+ There are at most $Dq$ independent trials, each producing a random list
74
+ of at most $D$ shapes from $\mathcal F$. Delete every point on any listed
75
+ shape, and denote the surviving set by $X$. Assume that
76
+ \begin{enumerate}
77
+ \item for each point $x$ and each trial, the probability that this
78
+ trial deletes $x$ is at most $D/q$;
79
+ \item $\Pr(x\in X)=\delta_q\geq\delta$ for every $x\in\F_q^2$;
80
+ \item for each affine line $\ell$, the sum over trials of the
81
+ probabilities that the trial lists the exact shape $\ell$ is
82
+ at most $D/q$.
83
+ \end{enumerate}
84
+ Write $X^\ell$ for the surviving set when all exact occurrences of the
85
+ shape $\ell$ are ignored, with every other listed shape still deleted.
86
+ With probability tending to one, both of the following statements
87
+ hold:
88
+ \begin{enumerate}
89
+ \item $|X^\ell\cap\ell|\geq\delta q/2$ for every affine line $\ell$;
90
+ \item every set of at most $q$ affine lines covering all but at most
91
+ $2q$ points of $X$ contains at least $(1-\rho)q$ lines through a
92
+ common projective point.
93
+ \end{enumerate}
94
+ \end{lemma}
95
+
96
+ \begin{proof}
97
+ We first establish a simultaneous lower bound on surviving
98
+ cross-intersections for every admissible pair of short line lists,
99
+ ignoring any deletion shape equal to one of those lines. After fixing
100
+ such a realization, we show that any cover lacking an almost full
101
+ pencil contains an admissible pair with too few surviving
102
+ cross-intersections. This second step samples only within the fixed
103
+ cover, with separate arguments according to its maximum concurrency.
104
+
105
+ Fix the absolute constant $\kappa\in(0,1/10)$ of
106
+ Theorem~\ref{thm:incidence}, and put $\epsilon=\kappa/10$.
107
+ All constants below may depend on the fixed parameters, but not on
108
+ $q$, the particular deletion distributions, or a subsequently chosen
109
+ cover.
110
+
111
+ \paragraph{Uniform point and line counts.}
112
+ Expose the independent trials one at a time. Changing one trial
113
+ changes $|X|$ by at most $2D^2q$, because the old and new lists contain
114
+ at most $2D$ shapes in total and each has at most $Dq$ points.
115
+ The exposure observation in~\cite[Lemma~A.3]{OpenAI2026Balanced}
116
+ therefore bounds the absolute martingale increment by $L=2D^2q$.
117
+ There are $T\le Dq$ trials, and $\E|X|=\delta_q q^2$. The fixed-time
118
+ concentration estimate in~\cite[Lemma~A.2]{OpenAI2026Balanced}, with
119
+ $u=q^{3/2+\epsilon}$, gives
120
+ \[
121
+ \Pr\bigl(\bigl||X|-\delta_q q^2\bigr|\ge q^{3/2+\epsilon}\bigr)
122
+ \le2\exp\left(-\frac{q^{2\epsilon}}{32D^5}\right).
123
+ \]
124
+ If there are no trials, the count is deterministic and this bound
125
+ holds as well. Equivalently, we may add a dummy trial of zero change.
126
+
127
+ For the line count $|X^\ell\cap\ell|$, the rule ignoring exact copies
128
+ of $\ell$ is applied separately to each trial. Changing one trial
129
+ then changes the count by at most $2D^2$: each of its at most $2D$
130
+ old or new shapes meets $\ell$ in at most $D$ points. With
131
+ $L=2D^2$ and $u=q^{1/2+\epsilon}$, the same two elementary estimates
132
+ and $T\le Dq$ give
133
+ \[
134
+ \Pr\bigl(\bigl||X^\ell\cap\ell|-\E|X^\ell\cap\ell|\bigr|
135
+ \ge q^{1/2+\epsilon}\bigr)
136
+ \le2\exp\left(-\frac{q^{2\epsilon}}{32D^5}\right).
137
+ \]
138
+
139
+ Moreover, a point restored by ignoring $\ell$ can be restored only if
140
+ some trial lists $\ell$ exactly. The probability of this event is at
141
+ most $D/q$, by the third deletion hypothesis. Therefore
142
+ \[
143
+ \delta_q q\leq \E|X^\ell\cap\ell|\leq\delta_q q+D.
144
+ \]
145
+ There are $q(q+1)$ affine lines. The superpolynomial tails and a union
146
+ bound consequently show that, with probability tending to one,
147
+ \begin{equation}\label{eq:lc-counts}
148
+ \begin{split}
149
+ |X|&=\delta_q q^2+O_D(q^{3/2+\epsilon}),\\
150
+ |X^\ell\cap\ell|&=\delta_q q+O_D(q^{1/2+\epsilon})
151
+ \qquad\text{for every affine line }\ell.
152
+ \end{split}
153
+ \end{equation}
154
+ The lower line estimate proves the first conclusion of the lemma.
155
+ For the pencil conclusion we will also need to bound overlaps in an
156
+ alleged cover. The same estimates give the uniform upper bound
157
+ \begin{equation}\label{eq:lc-line-upper}
158
+ |X\cap\ell|\leq\delta_q q+O_D(q^{1/2+\epsilon}),
159
+ \end{equation}
160
+ because $X\subseteq X^\ell$.
161
+
162
+ \paragraph{A simultaneous event for small line samples.}
163
+ The counts just proved control a single line but do not yet restrict
164
+ how a cover's lines meet. We now obtain a stronger test on short lists
165
+ of lines: provided their intersections are distinct and not concentrated
166
+ on a deletion shape, many of those intersections survive. The list
167
+ length will be logarithmic in $q$, so that the variance-sensitive tail
168
+ can pay for a union bound over all lists.
169
+
170
+ Set
171
+ \[
172
+ h=10(D+1),\qquad H_0=2Dh,\qquad
173
+ t=\lceil A\log q\rceil,
174
+ \]
175
+ where the fixed constant $A$ will be chosen below. Consider any ordered
176
+ tuple of $2t$ distinct affine lines, separated into two lists of length
177
+ $t$. Call the tuple admissible if its cross-list intersections form a
178
+ set $P_0$ of $t^2$ distinct finite points, and
179
+ \begin{equation}\label{eq:lc-occupancy}
180
+ |F\cap P_0|\leq H_0
181
+ \quad\text{for every }F\in\mathcal F
182
+ \text{ which is not one of the tuple lines}.
183
+ \end{equation}
184
+ For this tuple, ignore deletions by every shape equal to a tuple line,
185
+ and let $Y_0$ count the survivors in $P_0$ after the remaining deletions.
186
+ We claim that, with probability tending to one,
187
+ \begin{equation}\label{eq:lc-tuple-event}
188
+ Y_0\geq\frac{\delta t^2}{2}
189
+ \qquad\text{for every admissible tuple}.
190
+ \end{equation}
191
+
192
+ To prove the claim, fix a tuple in advance. Omitting shapes is a
193
+ deterministic operation on each trial, so the trials remain
194
+ independent. Omission can only restore points, and hence
195
+ $\E Y_0\geq\delta t^2$. By \eqref{eq:lc-occupancy}, each trial's
196
+ contribution to the deletion set within $P_0$ has size at most
197
+ $C_0=DH_0$. The probability that this contribution is nonempty is at
198
+ most $Dt^2/q$, by a union bound over $P_0$ and the per-point deletion
199
+ hypothesis.
200
+
201
+ For completeness, the rarity of a nonempty contribution also controls
202
+ the conditional variance of the exposure martingale. Fix the past,
203
+ and let $g_i(w)$ be the conditional expected final value of $Y_0$ when
204
+ the current trial has outcome $w$. Let $g_i(\varnothing)$ denote the
205
+ hypothetical value obtained by making this trial delete nothing on
206
+ $P_0$. Independence leaves the law of the future trials unchanged, so
207
+ \[
208
+ |g_i(w)-g_i(\varnothing)|\leq C_0,
209
+ \]
210
+ with equality to zero whenever the trial's contribution is empty.
211
+ The current trial also retains its original law conditional on the
212
+ past. Thus the martingale increment has absolute value at most $2C_0$, and
213
+ its conditional variance is at most
214
+ \[
215
+ \E\bigl((g_i(w)-g_i(\varnothing))^2\mid\text{past}\bigr)
216
+ \leq C_0^2\frac{Dt^2}{q}.
217
+ \]
218
+ The sum of conditional variances is at most $D^2C_0^2t^2$, since there
219
+ are at most $Dq$ trials. Applying Lemma~\ref{lem:martingale} at deviation
220
+ $\delta t^2/2$ yields
221
+ \begin{equation}\label{eq:lc-tuple-tail}
222
+ \Pr\left(Y_0<\frac{\delta t^2}{2}\right)
223
+ \leq2e^{-c_0t^2},\qquad
224
+ c_0=\min\left\{\frac{\delta^2}{16D^2C_0^2},
225
+ \frac{\delta}{16C_0}\right\}>0.
226
+ \end{equation}
227
+ In particular, $c_0$ is independent of $A$.
228
+
229
+ There are at most $(q(q+1))^{2t}$ ordered tuples. The logarithm of the
230
+ union bound in \eqref{eq:lc-tuple-tail} is
231
+ \[
232
+ -c_0t^2+4t\log q+O(t/q)+O(1)
233
+ =\bigl(-c_0A^2+4A+o(1)\bigr)(\log q)^2.
234
+ \]
235
+ Choose, for example, any fixed $A>5/c_0$. This proves
236
+ \eqref{eq:lc-tuple-event} simultaneously for all admissible tuples.
237
+
238
+ \paragraph{Consequences of an alleged cover.}
239
+ The random part of the argument is complete. We now keep the deletion
240
+ outcome fixed and show deterministically that the simultaneous events
241
+ exclude any cover without an almost full pencil. Random sampling below
242
+ is only a way to find a short witness inside a fixed cover.
243
+
244
+ Fix a realization satisfying both \eqref{eq:lc-counts} and
245
+ \eqref{eq:lc-tuple-event}. Suppose that the second conclusion of the
246
+ lemma fails. From an offending cover remove every line which actually
247
+ occurred as a listed deletion shape. Such a line contains no point of
248
+ $X$, so the remaining line set $L$ still covers all but at most $2q$
249
+ points of $X$. Put $m=|L|$, and for any projective point $p$ write
250
+ $n_p=|\{\ell\in L:p\in\ell\}|$. Define
251
+ \[
252
+ E_L=\sum_{x\in X}(n_x-1)_+,
253
+ \qquad (a)_+=\max\{a,0\}.
254
+ \]
255
+ The count of covered survivors and \eqref{eq:lc-line-upper} give
256
+ \[
257
+ m\bigl(\delta_q q+O_D(q^{1/2+\epsilon})\bigr)
258
+ \geq\delta_q q^2-O_D(q^{3/2+\epsilon})-2q.
259
+ \]
260
+ Since $\delta_q\geq\delta$ and $m\leq q$, this implies
261
+ \begin{equation}\label{eq:lc-cover-counts}
262
+ m=q-O_{D,\delta}(q^{1/2+\epsilon}),\qquad
263
+ E_L=O_D(q^{3/2+\epsilon}).
264
+ \end{equation}
265
+ For the second estimate, subtract the number of covered survivors
266
+ from $\sum_{\ell\in L}|X\cap\ell|$ and use $m\leq q$.
267
+ Finally, put
268
+ \[
269
+ R=\max_{p\in\PP^2(\F_q)}n_p.
270
+ \]
271
+ The failure of the pencil conclusion implies $R\leq(1-\rho)q$.
272
+ We will find an admissible tuple of lines from $L$ with fewer than
273
+ $\delta t^2/2$ survivors in its cross-intersection set.
274
+
275
+ \paragraph{Low concurrency: $R\leq q^{1/2+\kappa/4}$.}
276
+ Let $T=q^{1/2-\kappa/3}$. The number of ordered pairs of distinct lines
277
+ of $L$ meeting at a point $x\in X$ is $\sum_{x\in X}n_x(n_x-1)$.
278
+ Points with $n_x<T$ contribute at most
279
+ \begin{equation}\label{eq:lc-low-light}
280
+ T E_L=O(q^{2-7\kappa/30}).
281
+ \end{equation}
282
+ The set $P=\{x\in X:n_x\geq T\}$ has size
283
+ \[
284
+ |P|\leq\frac{E_L}{T-1}
285
+ =O(q^{1+13\kappa/30})\leq q^{1+\kappa}
286
+ \]
287
+ for sufficiently large $q$. Theorem~\ref{thm:incidence}, applied to
288
+ $P$ and $L$, therefore gives $\sum_{x\in P}n_x\leq q^{3/2-\kappa}$.
289
+ The contribution of these points to the ordered-pair count is at most
290
+ \begin{equation}\label{eq:lc-low-heavy}
291
+ R\sum_{x\in P}n_x\leq q^{2-3\kappa/4}.
292
+ \end{equation}
293
+ Together, \eqref{eq:lc-low-light} and \eqref{eq:lc-low-heavy} show that
294
+ the fraction of ordered distinct line pairs meeting in $X$ is
295
+ \begin{equation}\label{eq:lc-low-pair-fraction}
296
+ O\bigl(q^{-7\kappa/30}+q^{-3\kappa/4}\bigr)=o(1).
297
+ \end{equation}
298
+
299
+ Sample an ordered tuple of $2t$ distinct lines uniformly from $L$.
300
+ The expected number of its cross pairs meeting in $X$ is $t^2$ times
301
+ the fraction in \eqref{eq:lc-low-pair-fraction}. Markov's inequality
302
+ shows that this number is less than $\delta t^2/2$ with probability
303
+ tending to one.
304
+
305
+ We next check the two admissibility conditions. A given sampled pair
306
+ is parallel with probability at most $R/(m-1)$. Once two distinct
307
+ lines have been sampled, at most $R$ population lines pass through
308
+ their projective intersection, so the probability of concurrency for
309
+ any specified three sampled positions is at most $R/(m-2)$. The
310
+ probability of any parallel pair or concurrent triple in the tuple
311
+ is consequently
312
+ \begin{equation}\label{eq:lc-low-degeneracy}
313
+ O\left(\frac{(t^2+t^3)R}{m}\right)
314
+ =O\bigl((\log q)^3q^{-1/2+\kappa/4}\bigr)=o(1).
315
+ \end{equation}
316
+ If neither event occurs, every cross intersection is finite and the
317
+ cross intersections are distinct: equality of two different cross
318
+ intersections would make at least three of the tuple lines concurrent.
319
+
320
+ To verify \eqref{eq:lc-occupancy}, fix $F\in\mathcal F$. Consider the
321
+ event that $F$ is not a tuple line but contains more than $H_0$ distinct
322
+ finite cross intersections. Each tuple line then contains at most
323
+ $D$ points of $F$. Greedily choose a cross intersection on $F$ and its
324
+ two representing positions, and discard all cross intersections on
325
+ either of those lines. Each step discards at most $2D$ points. Since
326
+ $H_0=2Dh$, this produces $h$ cross pairs whose $2h$ positions are
327
+ distinct.
328
+
329
+ Among the population $L$, there are at most $mDR$ ordered distinct
330
+ line pairs, neither line equal to $F$, whose intersection lies in
331
+ $F$. Indeed, the first line meets $F$ in at most $D$ points, and at
332
+ each such point there are at most $R$ choices of the second line.
333
+ There are at most $t^{2h}$ ordered choices of the $h$ cross pairs of
334
+ positions. For each choice, the sampled lines at those $2h$ distinct
335
+ positions are uniform among $(m)_{2h}$ assignments, where
336
+ $(z)_a=z(z-1)\cdots(z-a+1)$. The probability of the event for this
337
+ fixed shape is therefore at most
338
+ \begin{equation}\label{eq:lc-low-shape}
339
+ \frac{t^{2h}(mDR)^h}{(m)_{2h}}
340
+ =O_{D,h}\left(\left(\frac{t^2R}{m}\right)^h\right).
341
+ \end{equation}
342
+ The numerator may count assignments with repeated population lines;
343
+ this only enlarges the upper bound. Summing
344
+ \eqref{eq:lc-low-shape} over all shapes gives
345
+ \[
346
+ O\bigl((\log q)^{2h}q^{D-h(1/2-\kappa/4)}\bigr)=o(1),
347
+ \]
348
+ because $\kappa<1/10$ and $h=10(D+1)$ imply
349
+ \[
350
+ D-h(1/2-\kappa/4)
351
+ <D-\frac{19}{4}(D+1)<0.
352
+ \]
353
+ Thus, with probability tending to one, the sampled tuple is admissible
354
+ and has fewer than $\delta t^2/2$ cross pairs meeting in $X$.
355
+
356
+ \paragraph{High concurrency: $R>q^{1/2+\kappa/4}$.}
357
+ Choose a projective point $p$ with $n_p=R$, and take all $R$ lines of
358
+ $L$ through $p$ as the pencil. Its complement has size
359
+ \[
360
+ N=m-R\geq\rho q/2
361
+ \]
362
+ for sufficiently large $q$, by \eqref{eq:lc-cover-counts}; no
363
+ complement line passes through $p$. Sample the first list of $t$ lines
364
+ uniformly without replacement from the pencil, and independently
365
+ sample the second list in the same way from the complement.
366
+
367
+ Any cross intersection lies off $p$. At a cross intersection
368
+ $x\in X$, exactly one pencil line passes through $x$, and the number
369
+ of cross pairs meeting there is the number of complement lines
370
+ through $x$, namely $n_x-1$. Thus at most $E_L$ of all $RN$ population
371
+ cross pairs meet in $X$. Their fraction is at most
372
+ \begin{equation}\label{eq:lc-high-pair-fraction}
373
+ \frac{E_L}{RN}
374
+ =O\bigl(q^{\epsilon-\kappa/4}\bigr)
375
+ =O(q^{-3\kappa/20})=o(1).
376
+ \end{equation}
377
+ As before, expectation and Markov's inequality show that fewer than
378
+ $\delta t^2/2$ sampled cross pairs meet in $X$, with probability
379
+ tending to one.
380
+
381
+ For a fixed complement line, at most one pencil line meets it at
382
+ infinity when $p$ is finite. When $p$ is at infinity, the pencil lines
383
+ have direction $p$ and every complement line has a different
384
+ direction, so all cross intersections are finite. The probability of
385
+ any infinite cross intersection is therefore at most $t^2/R$.
386
+ Two equal cross intersections must use the same pencil line, since
387
+ distinct pencil lines meet only at $p$, which lies on no complement
388
+ line. Given two complement lines, their projective intersection
389
+ determines at most one affine pencil line, namely its join with $p$.
390
+ If this join is the line at infinity, there is no affine candidate.
391
+ Conditioning on the second list and taking a union bound over its
392
+ pairs shows that the probability of a collision is $O(t^3/R)$.
393
+ The total probability of a failure of finiteness or distinctness is
394
+ therefore
395
+ \begin{equation}\label{eq:lc-high-degeneracy}
396
+ O\left(\frac{t^2+t^3}{R}\right)
397
+ =O\bigl((\log q)^3q^{-1/2-\kappa/4}\bigr)=o(1).
398
+ \end{equation}
399
+
400
+ Fix $F\in\mathcal F$, and consider the event that $F$ is not a tuple
401
+ line but contains more than $H_0$ distinct finite cross intersections.
402
+ The same greedy argument gives $h$ cross pairs with disjoint
403
+ positions. There are at most
404
+ $DN$ population cross pairs, with neither line equal to $F$, whose
405
+ intersection lies in $F$: a complement line distinct from $F$ meets
406
+ $F$ in at most $D$ points, all off $p$, and each such point determines
407
+ at most one pencil line. The two lists are sampled independently, so
408
+ the probability of this occupancy violation for a fixed shape is at
409
+ most
410
+ \begin{equation}\label{eq:lc-high-shape}
411
+ \frac{t^{2h}(DN)^h}{(R)_h(N)_h}
412
+ =O_{D,h}\left(\left(\frac{t^2}{R}\right)^h\right).
413
+ \end{equation}
414
+ After summing over $\mathcal F$, the bound becomes
415
+ \[
416
+ O\bigl((\log q)^{2h}q^{D-h(1/2+\kappa/4)}\bigr)=o(1),
417
+ \]
418
+ since
419
+ \[
420
+ D-h(1/2+\kappa/4)<D-5(D+1)<0.
421
+ \]
422
+ The sampled tuple is consequently admissible and has fewer than
423
+ $\delta t^2/2$ cross pairs meeting in $X$, with probability tending
424
+ to one in this regime as well.
425
+
426
+ \paragraph{The contradiction and the order of choices.}
427
+ All sampling estimates above are uniform over line sets satisfying
428
+ \eqref{eq:lc-cover-counts} and the appropriate bound on $R$. In either
429
+ regime, for every sufficiently large $q$ there is therefore an
430
+ admissible tuple from the fixed line set $L$ with
431
+ \[
432
+ |X\cap P_0|<\delta t^2/2.
433
+ \]
434
+ No line of $L$ actually occurred as a listed deletion shape. Hence
435
+ ignoring exact occurrences of its tuple lines changes none of the
436
+ deletions in the fixed realization, and the tuple's count $Y_0$ is
437
+ exactly $|X\cap P_0|$. This contradicts
438
+ \eqref{eq:lc-tuple-event}.
439
+
440
+ In particular, the cover and the tuple are allowed to depend on the
441
+ realized deletions: the event \eqref{eq:lc-tuple-event} was established
442
+ simultaneously for every admissible tuple before fixing the
443
+ realization. Sampling from $L$ is used only to prove the existence of
444
+ a tuple inside that fixed realization. No concentration estimate is
445
+ conditioned on the choice of the cover. The contradiction proves the
446
+ second conclusion, and finishes the proof.
447
+ \end{proof}
preprints/A-Counterexample-to-Rysers-Covering-Conjecture-September-23-2026/build/paper.tex ADDED
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+ \hypersetup{colorlinks=true,linkcolor=blue!45!black,citecolor=blue!45!black,
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+ pdftitle={A counterexample to Ryser's covering conjecture},pdfauthor={OpenAI}}
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+ \urlstyle{same}
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+ \setlength{\emergencystretch}{2em}
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+ \setlist{itemsep=3pt,topsep=5pt}
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+ \newtheorem{theorem}{Theorem}[section]
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+ \newtheorem{lemma}[theorem]{Lemma}
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+ \newtheorem{proposition}[theorem]{Proposition}
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+ \newtheorem{corollary}[theorem]{Corollary}
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+ \theoremstyle{remark}
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+ \newtheorem{remark}[theorem]{Remark}
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+ \newtheorem{definition}[theorem]{Definition}
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+ \newcommand{\F}{\mathbb F}
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+ \newcommand{\PP}{\mathbb P}
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+ \DeclareMathOperator{\Var}{Var}
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+ \DeclareMathOperator{\Cov}{Cov}
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+ \DeclareMathOperator{\supp}{supp}
40
+ \title{A counterexample to Ryser's covering conjecture}
41
+ \author{OpenAI}
42
+ \date{September 23, 2026}
43
+
44
+ \begin{document}
45
+ \maketitle
46
+ \begin{abstract}
47
+ For every sufficiently large prime $s\equiv2\pmod3$ and every sufficiently
48
+ large odd integer $n$, with the threshold depending on $s$, we construct
49
+ an intersecting $(s^n+1)$-partite $(s^n+1)$-uniform hypergraph with covering
50
+ number $s^n+1$. This disproves Ryser's covering conjecture in its
51
+ intersecting case.
52
+ \end{abstract}
53
+
54
+ \section{Introduction}
55
+
56
+ A vertex cover of a finite hypergraph $H$ is a set of vertices meeting
57
+ every edge. Its covering number $\tau(H)$ is the minimum size of such a
58
+ set, and its matching number $\nu(H)$ is the maximum number of pairwise
59
+ disjoint edges. For an integer $r\ge2$, an $r$-partite $r$-uniform
60
+ hypergraph has disjoint vertex parts $V_1,\ldots,V_r$, with every edge
61
+ containing exactly one vertex from each part. Ryser's covering
62
+ conjecture asserts that every such hypergraph satisfies
63
+ \begin{equation}\label{eq:ryser}
64
+ \tau(H)\le(r-1)\nu(H).
65
+ \end{equation}
66
+ A nonempty hypergraph is intersecting when every two distinct edges
67
+ meet; equivalently, its matching number is one. In this case the
68
+ conjecture asks for a cover of size at most $r-1$. The vertices of a
69
+ cover may lie in several different parts, which is the central
70
+ obstacle in constructing a counterexample.
71
+
72
+ For $r=2$, inequality~\eqref{eq:ryser} is K\H{o}nig's matching theorem.
73
+ An equivalent formulation appears in Henderson's 1971
74
+ thesis~\cite{Henderson1971}; Best and Wanless discuss the history of its
75
+ attribution to Ryser~\cite{BestWanless2018}. Aharoni proved the full
76
+ tripartite case~\cite{Aharoni2001}. In the intersecting case, the results
77
+ through rank four are due to Gy\'arf\'as, and the rank-five result to
78
+ Tuza, as recorded by Kir\'aly and T\'othm\'er\'esz~\cite{KiralyTothmeresz2017};
79
+ see also Tuza's early study of the covering conjecture~\cite{Tuza1983}.
80
+ Haxell and Scott proved $\tau(H)\le(r-\epsilon)\nu(H)$ for some
81
+ $\epsilon>0$ when $r=4$ or $5$, without assuming
82
+ intersection~\cite{HaxellScott2012}. White proved the particular
83
+ rank-four case $\nu(H)=2$, obtaining $\tau(H)\le6$~\cite{White2026}.\footnote{White
84
+ reports assistance from GPT-5.6 Sol and Claude in the Methods section
85
+ of his preprint.}
86
+ Under the additional assumption that any two distinct edges meet in
87
+ exactly one vertex, Franceti\'{c}, Herke, McKay, and Wanless established
88
+ the intersecting case through rank nine~\cite{FranceticHerkeMcKayWanless2017}.
89
+ Bishnoi, Das, Morris, and Szab\'o obtained bounds when every pair of
90
+ edges has a larger prescribed intersection~\cite{BDMS2021}.
91
+
92
+ Finite planes supply the classical equality examples. Delete a point
93
+ and all lines through it from a projective plane of order $q$. Partition
94
+ the remaining points according to the deleted line through them, and
95
+ take the remaining lines as hyperedges. The result is intersecting,
96
+ has $q+1$ parts and covering number $q$. Thus equality in the proposed
97
+ bound occurs whenever $r-1$ is a prime power. Work of Mansour, Song, and
98
+ Yuster~\cite{MansourSongYuster2009} and Aharoni, Bar\'{a}t, and
99
+ Wanless~\cite{AharoniBaratWanless2016} studies the structure and sparsity
100
+ of equality examples. Abu-Khazneh, Bar\'{a}t, Pokrovskiy, and
101
+ Szab\'{o} exploit the rigidity of minimum covers in a truncated plane
102
+ and add exceptional edges to obtain further equality
103
+ examples~\cite{AbuKhaznehBaratPokrovskiySzabo2019}. In that construction,
104
+ the number of parts and the covering number both increase by one.
105
+ Haxell and Scott combine affine planes with intersecting configurations
106
+ to obtain covering number at least $r-4$ for every sufficiently large
107
+ $r$, improved to $r-3$ when $r$ is even~\cite{HaxellScott2017}.
108
+
109
+ Our construction also starts from a finite plane and inserts exceptional
110
+ edges, but keeps one part for each ambient direction. It changes the
111
+ line labels within these parts to raise the covering number beyond
112
+ $q$. The following theorem gives the precise field orders for which
113
+ this can be done.
114
+
115
+ \begin{theorem}\label{thm:main}
116
+ There exists $s_0$ such that, for every prime $s\ge s_0$ with
117
+ $s\equiv2\pmod3$, there is an integer $n_0(s)\ge3$ with the following
118
+ property. For every odd integer $n\ge n_0(s)$, put $q=s^n$.
119
+ There is a finite intersecting $(q+1)$-partite $(q+1)$-uniform
120
+ hypergraph $H$ satisfying
121
+ \[
122
+ \tau(H)=q+1.
123
+ \]
124
+ In particular, the intersecting case of~\eqref{eq:ryser} is false.
125
+ \end{theorem}
126
+
127
+ Every edge of a nonempty intersecting hypergraph is itself a cover,
128
+ so the assertion $\tau(H)\le q+1$ is automatic. The proof must construct
129
+ an intersecting hypergraph and exclude every cover of size at most $q$.
130
+ We first fix any sufficiently large eligible prime $s$, construct a
131
+ configuration in $\F_s^2$, and then take $n$ sufficiently large among
132
+ the odd integers. All subsequent thresholds may depend on that fixed
133
+ configuration. The result is asymptotic; the proof does not give a
134
+ numerical threshold.
135
+
136
+ A companion paper~\cite{OpenAI2026Balanced} proves a different theorem:
137
+ for every sufficiently large prime $q$, it constructs such a hypergraph
138
+ with exactly $q+1$ vertices in every part and with every vertex
139
+ nonisolated. Its construction modifies line partitions directly in the
140
+ prime plane. Here the field order is a proper odd power, and the proof
141
+ uses a small-field configuration with a nonlinear change of
142
+ coordinates. The two constructions give distinct ranges of ranks.
143
+ The only results imported from the companion are its three elementary
144
+ estimates in Appendix~A: the affine second-moment identity
145
+ (Lemma~A.1), bounded-drift concentration (Lemma~A.2), and the exposure
146
+ bound for independent trials (Lemma~A.3).
147
+
148
+ Lov\'asz proposed the stronger assertion that deleting $r-1$ vertices
149
+ can always reduce the matching number. Clow, Haxell, and Mohar
150
+ disproved that assertion at $r=3$~\cite{CHM2025}; Abiad, Garbe, Povill,
151
+ and Spiegel subsequently gave an infinite family at $r=3$ and
152
+ examples at $r=4$~\cite{AbiadGarbePovillSpiegel2025}. These examples
153
+ are consistent with~\eqref{eq:ryser}. They exclude a prescribed
154
+ matching-reduction procedure, whereas Theorem~\ref{thm:main}
155
+ violates the covering inequality itself.
156
+
157
+ \subsection*{Monochromatic tree covers}
158
+
159
+ An $r$-edge-coloring here assigns exactly one of $r$ colors to each edge.
160
+ A monochromatic tree cover is a family of monochromatic trees whose vertex
161
+ sets cover the graph; the trees may overlap, and singleton trees are allowed.
162
+ Gy\'arf\'as's conjecture asks whether $r-1$ such trees suffice for every
163
+ $r$-edge-colored complete graph; see \cite[Conjecture~1]{Milicevic2017}.
164
+ This is the covering formulation recorded after Theorem~2 in
165
+ \cite[Section~3]{ErdosGyarfasPyber1991}, not the distinct vertex-disjoint
166
+ tree-partition conjecture numbered Conjecture~2 there.
167
+
168
+ \begin{corollary}\label{cor:tree-cover}
169
+ Let $s_0$ and $n_0(s)$ be as in Theorem~\ref{thm:main}. For every prime
170
+ $s\ge s_0$ with $s\equiv2\pmod3$ and every odd integer $n\ge n_0(s)$,
171
+ put $r=s^n+1$. There is a finite simple complete graph with an
172
+ $r$-edge-coloring for which the minimum number of monochromatic trees
173
+ needed to cover its vertices is exactly $r$. The same minimum holds with
174
+ connected monochromatic subgraphs or maximal monochromatic components in
175
+ place of trees.
176
+ \end{corollary}
177
+
178
+ \begin{proof}
179
+ Take the hypergraph $H$ from Theorem~\ref{thm:main}, with parts
180
+ $V_1,\ldots,V_r$. For $e\in E(H)$, let $x_i(e)$ be the unique vertex in
181
+ $e\cap V_i$. Form the complete graph $K$ with vertex set $E(H)$. For each
182
+ pair of distinct hyperedges $e,f$, choose one index $i$ with
183
+ $x_i(e)=x_i(f)$ and color the edge $ef$ by $i$. Such an index exists
184
+ because $H$ is intersecting. Only one color is chosen even when the two
185
+ hyperedges meet in several parts.
186
+
187
+ Along a color-$i$ path, the value of $x_i$ is constant. Thus every connected
188
+ color-$i$ subgraph determines a vertex of $V_i$ belonging to every
189
+ hyperedge indexed by that subgraph. For a singleton, choose any color and
190
+ the corresponding vertex of its hyperedge. If $t$ connected monochromatic
191
+ subgraphs cover the vertices of $K$, the at most $t$ hypergraph vertices so
192
+ chosen meet every edge of $H$. Hence $t\ge\tau(H)=r$.
193
+
194
+ Conversely, fix a vertex of $K$. The $r$ monochromatic stars centered there,
195
+ one for each color and allowing singleton stars, cover all vertices of $K$.
196
+ They give a tree cover of size at most $r$. The lower bound applies to trees
197
+ and to maximal monochromatic components as well, and the stars can be
198
+ enlarged to maximal components. This proves all three stated minima.
199
+ \end{proof}
200
+
201
+ Thus Gy\'arf\'as's cover conjecture fails at these extension-field ranks.
202
+ The examples admit no cover by $r-1$ connected monochromatic subgraphs even
203
+ without a diameter restriction. They therefore also refute Mili\'cevi\'c's
204
+ bounded-diameter strengthening \cite[Conjecture~6]{Milicevic2017}, whose
205
+ diameter bound may depend on $r$, and the $\alpha=1$ case of the conjecture
206
+ of DeBiasio, Kamel, McCourt, and Sheats
207
+ \cite[Conjecture~2.8]{DeBiasioKamelMcCourtSheats2021}, whose diameter bound
208
+ depends only on the independence number $\alpha$. Indeed, $\alpha(K)=1$,
209
+ so the latter conjecture also demands a cover by at most $r-1$ such
210
+ subgraphs.
211
+
212
+ \subsection*{Proof strategy}
213
+
214
+ In the affine-plane model, the parts are indexed by the $q+1$ directions
215
+ in $\F_q^2$, and the vertices of a part are the $q$ lines of that
216
+ direction. A point $x$ defines an edge consisting of its incident line
217
+ in each direction. The edges of two points intersect at their join,
218
+ but a full parallel class always gives a cover of size $q$. We retain
219
+ many of these point edges and add exceptional edges whose labels are
220
+ changed in some directions. The construction has three tasks: preserve
221
+ intersection, restrict small covers of the retained point edges, and
222
+ make the exceptional edges too costly for those covers.
223
+
224
+ \paragraph{Restricting the ordinary cover.}
225
+ Delete a bounded number of translated shapes in each of $O(q)$
226
+ independent trials. The shapes are lines or curves that meet every
227
+ line in boundedly many points. Thus a shape has bounded intersection
228
+ with a line unless it is that line itself. Section~\ref{sec:linecover} proves that, under explicit
229
+ uniform survival assumptions, every cover of almost all surviving
230
+ points by at most $q$ lines contains almost a pencil. Here a pencil is
231
+ a family of lines through one projective point, including a parallel
232
+ class when that point is at infinity. Surviving points on each
233
+ nondeleted line then force every nondeleted member of this pencil
234
+ into the cover. To obtain the pencil statement over the required
235
+ extension fields, Section~\ref{sec:incidence} first proves an incidence
236
+ saving by the sum--product method of Bourgain, Katz, and
237
+ Tao~\cite{BKT2004}. Its constants are uniform over fields whose proper
238
+ subfields all have order at most $q^{1/3}$.
239
+
240
+ \paragraph{One configuration in two coordinates.}
241
+ In a fixed prime plane $\F_s^2$, remove one line in each finite nonzero
242
+ direction and call the remaining set $Y$. The change of coordinates
243
+ $f(x,y)=(x^3,y)$ is bijective when $s\equiv2\pmod3$. Original line
244
+ labels determine which ambient point edges must be deleted to
245
+ intersect the exceptional edges. The labels for altered directions
246
+ are instead read from the lines through $f(w)$, for $w\in Y$.
247
+ The map $f$ preserves the horizontal and vertical parallel classes;
248
+ this ensures intersection within the exceptional configuration.
249
+ Its nonlinear action on the other lines makes their images curves
250
+ with at most three intersections with any line. Applying the deletion
251
+ lemma in these new coordinates yields the crucial obstruction:
252
+ covering $f(Y)$ by $a$ lines and $b$ individual points with
253
+ $a+b/2\le s$ requires exactly one full parallel class and no point
254
+ resources. Section~\ref{sec:gadget} proves this statement together
255
+ with the ordinary-coordinate occupancy needed later.
256
+
257
+ \paragraph{Placing the configurations and spending the cover budget.}
258
+ Embed linearly transformed copies of $Y$ in $\F_q^2$ so that every
259
+ ambient direction is altered in one or two copies. Arbitrary translates
260
+ could create disjoint exceptional edges. We therefore sample a fixed
261
+ number of independent candidate translates for each copy.
262
+ Section~\ref{sec:selection} proves that one can choose compatible
263
+ representatives from these pools, using an independent-transversal
264
+ argument in the tradition of Haxell~\cite{Haxell1995,Haxell2001}.
265
+ Section~\ref{sec:placement} proves the deletion estimates for the
266
+ entire independent pool before making this selection. Keeping only
267
+ the selected deletions restores ordinary points, so the needed
268
+ estimates transfer by deterministic inclusion.
269
+
270
+ Section~\ref{sec:hypergraph} gives the labels of every edge, proves
271
+ intersection, and excludes a cover of size at most $q$. After the
272
+ ordinary edges force a pencil, its center determines the remaining
273
+ argument. At infinity, the uncovered exceptional configurations
274
+ require more vertices than the missing parallel lines release.
275
+ Inside an embedded configuration, the remaining budget would cover
276
+ $f(Y)$ by at most $s$ lines including two nonparallel axis lines.
277
+ Outside every configuration, each deleted pencil line supplies five
278
+ uncovered exceptional edges, while every additional vertex covers at
279
+ most five. In all three cases the available budget is too small.
280
+
281
+ \paragraph{Conventions.}
282
+ A direction is a one-dimensional linear subspace of $\F_q^2$; as a subspace
283
+ it includes zero. The projective completion adds one point at infinity per
284
+ direction. A pencil consists of the affine lines through a projective point:
285
+ it has $q+1$ members for a finite center and $q$ members for a center at
286
+ infinity. Thus concurrence always includes parallel lines.
287
+ For a positive integer $j$, write $(a)_j=a(a-1)\cdots(a-j+1)$.
288
+ All asymptotic constants may depend on the parameters explicitly held fixed.
289
+ An event holds with high probability if its probability tends to one along
290
+ the specified sequence of fields. The small field is fixed before the
291
+ ambient field tends to infinity.
292
+
293
+ \input{incidence}
294
+ \input{linecover}
295
+ \input{selection}
296
+ \input{construction}
297
+
298
+ \Needspace{32\baselineskip}
299
+ \bibliographystyle{plain}
300
+ \bibliography{references}
301
+ \end{document}
preprints/A-Counterexample-to-Rysers-Covering-Conjecture-September-23-2026/build/references.bib ADDED
@@ -0,0 +1,390 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ @phdthesis{Henderson1971,
2
+ author = {Henderson, John Robert},
3
+ title = {Permutation Decompositions of {(0,1)}-Matrices and Decomposition Transversals},
4
+ school = {California Institute of Technology},
5
+ year = {1971},
6
+ doi = {10.7907/J1Z1-SK19},
7
+ note = {\href{https://doi.org/10.7907/J1Z1-SK19}{doi:10.7907/J1Z1-SK19}},
8
+ url = {https://thesis.caltech.edu/5726/}
9
+ }
10
+
11
+ @article{Aharoni2001,
12
+ author = {Aharoni, Ron},
13
+ title = {{Ryser}'s conjecture for tripartite 3-graphs},
14
+ journal = {Combinatorica},
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22
+ }
23
+
24
+ @article{Tuza1983,
25
+ author = {Tuza, Zsolt},
26
+ title = {{Ryser}'s conjecture on transversals of {$r$}-partite hypergraphs},
27
+ journal = {Ars Combinatoria},
28
+ volume = {16B},
29
+ pages = {201--209},
30
+ year = {1983},
31
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32
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33
+ }
34
+
35
+ @article{BDMS2021,
36
+ author = {Bishnoi, Anurag and Das, Shagnik and Morris, Patrick and Szab{\'o}, Tibor},
37
+ title = {{Ryser}'s conjecture for {$t$}-intersecting hypergraphs},
38
+ journal = {Journal of Combinatorial Theory, Series A},
39
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40
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41
+ year = {2021},
42
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43
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44
+ eprint = {2001.04132},
45
+ archivePrefix = {arXiv},
46
+ primaryClass = {math.CO},
47
+ url = {https://arxiv.org/abs/2001.04132}
48
+ }
49
+
50
+ @article{BKT2004,
51
+ author = {Bourgain, Jean and Katz, Nets and Tao, Terence},
52
+ title = {A sum-product estimate in finite fields, and applications},
53
+ journal = {Geometric and Functional Analysis},
54
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55
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56
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57
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58
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59
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60
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61
+ archivePrefix = {arXiv},
62
+ primaryClass = {math.CO},
63
+ url = {https://arxiv.org/abs/math/0301343}
64
+ }
65
+
66
+ @article{Petridis2012,
67
+ author = {Petridis, Giorgis},
68
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69
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70
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71
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72
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73
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74
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75
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76
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77
+ archivePrefix = {arXiv},
78
+ primaryClass = {math.CO},
79
+ url = {https://arxiv.org/abs/1101.3507}
80
+ }
81
+
82
+ @article{Haxell1995,
83
+ author = {Haxell, P. E.},
84
+ title = {A condition for matchability in hypergraphs},
85
+ journal = {Graphs and Combinatorics},
86
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87
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88
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89
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90
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91
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92
+ url = {https://doi.org/10.1007/BF01793010}
93
+ }
94
+
95
+ @article{CHM2025,
96
+ author = {Clow, Alexander and Haxell, Penny and Mohar, Bojan},
97
+ title = {A Counterexample to a Conjecture of {Lov{\'a}sz}},
98
+ journal = {Combinatorica},
99
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100
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101
+ year = {2026},
102
+ doi = {10.1007/s00493-026-00220-3},
103
+ note = {Article 26. \href{https://doi.org/10.1007/s00493-026-00220-3}{doi:10.1007/s00493-026-00220-3}},
104
+ eprint = {2505.05339},
105
+ archivePrefix = {arXiv},
106
+ primaryClass = {math.CO},
107
+ url = {https://link.springer.com/article/10.1007/s00493-026-00220-3}
108
+ }
109
+
110
+
111
+ @misc{BestWanless2018,
112
+ author = {Best, Darcy and Wanless, Ian M.},
113
+ title = {What did {Ryser} Conjecture?},
114
+ year = {2018},
115
+ eprint = {1801.02893},
116
+ archivePrefix = {arXiv},
117
+ primaryClass = {math.CO},
118
+ url = {https://arxiv.org/abs/1801.02893},
119
+ note = {\href{https://arxiv.org/abs/1801.02893}{arXiv:1801.02893}}
120
+ }
121
+
122
+ @article{HaxellScott2012,
123
+ author = {Haxell, P. E. and Scott, A. D.},
124
+ title = {On {Ryser}'s conjecture},
125
+ journal = {The Electronic Journal of Combinatorics},
126
+ volume = {19},
127
+ number = {1},
128
+ pages = {P23},
129
+ year = {2012},
130
+ doi = {10.37236/1175},
131
+ note = {\href{https://doi.org/10.37236/1175}{doi:10.37236/1175}}
132
+ }
133
+
134
+ @article{MansourSongYuster2009,
135
+ author = {Mansour, Toufik and Song, Chunwei and Yuster, Raphael},
136
+ title = {A comment on {Ryser}'s conjecture for intersecting hypergraphs},
137
+ journal = {Graphs and Combinatorics},
138
+ volume = {25},
139
+ number = {1},
140
+ pages = {101--109},
141
+ year = {2009},
142
+ doi = {10.1007/s00373-008-0821-9},
143
+ eprint = {0709.3138},
144
+ archivePrefix = {arXiv},
145
+ url = {https://arxiv.org/abs/0709.3138},
146
+ note = {\href{https://arxiv.org/abs/0709.3138}{arXiv:0709.3138}}
147
+ }
148
+
149
+ @article{AharoniBaratWanless2016,
150
+ author = {Aharoni, Ron and Bar{\'a}t, J{\'a}nos and Wanless, Ian M.},
151
+ title = {Multipartite hypergraphs achieving equality in {Ryser}'s conjecture},
152
+ journal = {Graphs and Combinatorics},
153
+ volume = {32},
154
+ number = {1},
155
+ pages = {1--15},
156
+ year = {2016},
157
+ doi = {10.1007/s00373-015-1575-9},
158
+ eprint = {1409.4833},
159
+ archivePrefix = {arXiv},
160
+ url = {https://arxiv.org/abs/1409.4833},
161
+ note = {\href{https://arxiv.org/abs/1409.4833}{arXiv:1409.4833}}
162
+ }
163
+
164
+ @article{FranceticHerkeMcKayWanless2017,
165
+ author = {Franceti{\'c}, Nevena and Herke, Sarada and McKay, Brendan D. and Wanless, Ian M.},
166
+ title = {On {Ryser}'s conjecture for linear intersecting multipartite hypergraphs},
167
+ journal = {European Journal of Combinatorics},
168
+ volume = {61},
169
+ pages = {91--105},
170
+ year = {2017},
171
+ doi = {10.1016/j.ejc.2016.10.004},
172
+ eprint = {1508.00951},
173
+ archivePrefix = {arXiv},
174
+ note = {\href{https://doi.org/10.1016/j.ejc.2016.10.004}{doi:10.1016/j.ejc.2016.10.004}}
175
+ }
176
+
177
+ @article{AbuKhaznehBaratPokrovskiySzabo2019,
178
+ author = {Abu-Khazneh, Ahmad and Bar{\'a}t, J{\'a}nos and Pokrovskiy, Alexey and Szab{\'o}, Tibor},
179
+ title = {A family of extremal hypergraphs for {Ryser}'s conjecture},
180
+ journal = {Journal of Combinatorial Theory, Series A},
181
+ volume = {161},
182
+ pages = {164--177},
183
+ year = {2019},
184
+ doi = {10.1016/j.jcta.2018.07.011},
185
+ eprint = {1605.06361},
186
+ archivePrefix = {arXiv},
187
+ note = {\href{https://doi.org/10.1016/j.jcta.2018.07.011}{doi:10.1016/j.jcta.2018.07.011}}
188
+ }
189
+
190
+ @article{HaxellScott2017,
191
+ author = {Haxell, P. E. and Scott, A. D.},
192
+ title = {A note on intersecting hypergraphs with large cover number},
193
+ journal = {The Electronic Journal of Combinatorics},
194
+ volume = {24},
195
+ number = {3},
196
+ pages = {P3.26},
197
+ year = {2017},
198
+ doi = {10.37236/6460},
199
+ eprint = {1609.05458},
200
+ archivePrefix = {arXiv},
201
+ note = {\href{https://doi.org/10.37236/6460}{doi:10.37236/6460}}
202
+ }
203
+
204
+ @incollection{Ruzsa1999,
205
+ author = {Ruzsa, Imre Z.},
206
+ title = {An analog of {Freiman}'s theorem in groups},
207
+ booktitle = {Structure theory of set addition},
208
+ series = {Ast{\'e}risque},
209
+ publisher = {Soci{\'e}t{\'e} Math{\'e}matique de France},
210
+ volume = {258},
211
+ pages = {323--326},
212
+ year = {1999},
213
+ url = {https://www.numdam.org/item/AST_1999__258__323_0/},
214
+ note = {\href{https://www.numdam.org/item/AST_1999__258__323_0/}{Primary source}}
215
+ }
216
+
217
+ @article{Gowers1998,
218
+ author = {Gowers, W. T.},
219
+ title = {A new proof of {Szemer{\'e}di}'s theorem for arithmetic progressions of length four},
220
+ journal = {Geometric and Functional Analysis},
221
+ volume = {8},
222
+ number = {3},
223
+ pages = {529--551},
224
+ year = {1998},
225
+ doi = {10.1007/s000390050065},
226
+ url = {https://doi.org/10.1007/s000390050065},
227
+ note = {\href{https://doi.org/10.1007/s000390050065}{doi:10.1007/s000390050065}}
228
+ }
229
+
230
+ @article{BalogSzemeredi1994,
231
+ author = {Balog, Antal and Szemer{\'e}di, Endre},
232
+ title = {A statistical theorem of set addition},
233
+ journal = {Combinatorica},
234
+ volume = {14},
235
+ number = {3},
236
+ pages = {263--268},
237
+ year = {1994},
238
+ doi = {10.1007/BF01212974},
239
+ url = {https://doi.org/10.1007/BF01212974},
240
+ note = {\href{https://doi.org/10.1007/BF01212974}{doi:10.1007/BF01212974}}
241
+ }
242
+
243
+ @article{FoxSudakov2011,
244
+ author = {Fox, Jacob and Sudakov, Benny},
245
+ title = {Dependent random choice},
246
+ journal = {Random Structures \& Algorithms},
247
+ volume = {38},
248
+ number = {1--2},
249
+ pages = {68--99},
250
+ year = {2011},
251
+ doi = {10.1002/rsa.20344},
252
+ eprint = {0909.3271},
253
+ archivePrefix = {arXiv},
254
+ url = {https://arxiv.org/abs/0909.3271},
255
+ note = {\href{https://arxiv.org/abs/0909.3271}{arXiv:0909.3271}}
256
+ }
257
+
258
+ @article{Haxell2001,
259
+ author = {Haxell, P. E.},
260
+ title = {A note on vertex list colouring},
261
+ journal = {Combinatorics, Probability and Computing},
262
+ volume = {10},
263
+ number = {4},
264
+ pages = {345--347},
265
+ year = {2001},
266
+ doi = {10.1017/S0963548301004758},
267
+ url = {https://doi.org/10.1017/S0963548301004758},
268
+ note = {\href{https://doi.org/10.1017/S0963548301004758}{doi:10.1017/S0963548301004758}}
269
+ }
270
+
271
+ @article{Freedman1975,
272
+ author={Freedman, David A.},
273
+ title={On tail probabilities for martingales},
274
+ journal={The Annals of Probability},
275
+ volume={3}, number={1}, pages={100--118}, year={1975},
276
+ doi={10.1214/aop/1176996452},
277
+ note = {\href{https://doi.org/10.1214/aop/1176996452}{doi:10.1214/aop/1176996452}}
278
+ }
279
+
280
+ @article{Jamison1977,
281
+ author={Jamison, Robert E.},
282
+ title={Covering finite fields with cosets of subspaces},
283
+ journal={Journal of Combinatorial Theory, Series A},
284
+ volume={22}, number={3}, pages={253--266}, year={1977},
285
+ doi={10.1016/0097-3165(77)90001-2},
286
+ note = {\href{https://doi.org/10.1016/0097-3165(77)90001-2}{doi:10.1016/0097-3165(77)90001-2}}
287
+ }
288
+
289
+ @article{BrouwerSchrijver1978,
290
+ author={Brouwer, A. E. and Schrijver, A.},
291
+ title={The blocking number of an affine space},
292
+ journal={Journal of Combinatorial Theory, Series A},
293
+ volume={24}, number={2}, pages={251--253}, year={1978},
294
+ doi={10.1016/0097-3165(78)90013-4},
295
+ note = {\href{https://doi.org/10.1016/0097-3165(78)90013-4}{doi:10.1016/0097-3165(78)90013-4}}
296
+ }
297
+
298
+ @article{BBS2010,
299
+ author={Blokhuis, A. and Brouwer, A. E. and Sz{\H o}nyi, T.},
300
+ title={Covering all points except one},
301
+ journal={Journal of Algebraic Combinatorics},
302
+ volume={32}, pages={59--66}, year={2010},
303
+ doi={10.1007/s10801-009-0204-1},
304
+ note = {\href{https://doi.org/10.1007/s10801-009-0204-1}{doi:10.1007/s10801-009-0204-1}}
305
+ }
306
+
307
+ @misc{White2026,
308
+ author = {White, Patrick},
309
+ title = {{Tuza}'s {Ryser}-conjecture claim for four-partite hypergraphs with matching number two},
310
+ year = {2026},
311
+ eprint = {2609.14281},
312
+ archivePrefix = {arXiv},
313
+ primaryClass = {math.CO},
314
+ note = {Version 1, 13 September 2026},
315
+ howpublished = {\href{https://arxiv.org/abs/2609.14281v1}{arXiv:2609.14281v1}},
316
+ url = {https://arxiv.org/abs/2609.14281v1}
317
+ }
318
+
319
+
320
+ @misc{OpenAI2026Balanced,
321
+ author = {{OpenAI}},
322
+ title = {{Balanced counterexamples to Ryser's conjecture at prime orders}},
323
+ howpublished = {OpenAI Math Release preprint
324
+ \href{https://github.com/openai/math/blob/main/preprints/Balanced-Counterexamples-to-Rysers-Conjecture-at-Prime-Orders-September-27-2026/paper.pdf}{OAI:Balanced-Counterexamples-to-Rysers-Conjecture-at-Prime-Orders-September-27-2026}},
325
+ year = {2026}
326
+ }
327
+
328
+ @misc{AbiadGarbePovillSpiegel2025,
329
+ author = {Abiad, Aida and Garbe, Frederik and Povill, Xavier and Spiegel, Christoph},
330
+ title = {Infinitely many counterexamples to a conjecture of {Lov{\'a}sz}},
331
+ year = {2025},
332
+ eprint = {2506.21286},
333
+ archivePrefix = {arXiv},
334
+ primaryClass = {math.CO},
335
+ note = {Version 2, 14 July 2025},
336
+ howpublished = {\href{https://arxiv.org/abs/2506.21286v2}{arXiv:2506.21286v2}},
337
+ url = {https://arxiv.org/abs/2506.21286v2}
338
+ }
339
+
340
+ @article{KiralyTothmeresz2017,
341
+ author = {Kir{\'a}ly, Zolt{\'a}n and T{\'o}thm{\'e}r{\'e}sz, Lilla},
342
+ title = {On {Ryser}'s Conjecture for $t$-Intersecting and Degree-Bounded Hypergraphs},
343
+ journal = {The Electronic Journal of Combinatorics},
344
+ volume = {24},
345
+ number = {4},
346
+ pages = {P4.40},
347
+ year = {2017},
348
+ doi = {10.37236/6448},
349
+ eprint = {1705.10024},
350
+ archivePrefix = {arXiv},
351
+ primaryClass = {math.CO},
352
+ note = {\href{https://doi.org/10.37236/6448}{doi:10.37236/6448}}
353
+ }
354
+
355
+ @article{ErdosGyarfasPyber1991,
356
+ author = {Erd{\H{o}}s, P. and Gy{\'a}rf{\'a}s, A. and Pyber, L.},
357
+ title = {Vertex coverings by monochromatic cycles and trees},
358
+ journal = {Journal of Combinatorial Theory, Series B},
359
+ volume = {51},
360
+ number = {1},
361
+ pages = {90--95},
362
+ year = {1991},
363
+ doi = {10.1016/0095-8956(91)90007-7},
364
+ note = {\href{https://doi.org/10.1016/0095-8956(91)90007-7}{doi:10.1016/0095-8956(91)90007-7}},
365
+ url = {https://doi.org/10.1016/0095-8956(91)90007-7}
366
+ }
367
+
368
+ @misc{Milicevic2017,
369
+ author = {Mili{\'c}evi{\'c}, Luka},
370
+ title = {Covering complete graphs by monochromatically bounded sets},
371
+ year = {2017},
372
+ eprint = {1705.09370},
373
+ archivePrefix = {arXiv},
374
+ primaryClass = {math.CO},
375
+ note = {Version 1, 25 May 2017},
376
+ howpublished = {\href{https://arxiv.org/abs/1705.09370v1}{arXiv:\allowbreak1705.09370v1}},
377
+ url = {https://arxiv.org/abs/1705.09370v1}
378
+ }
379
+
380
+ @misc{DeBiasioKamelMcCourtSheats2021,
381
+ author = {DeBiasio, Louis and Kamel, Yigal and McCourt, Grace and Sheats, Hannah},
382
+ title = {Generalizations and strengthenings of {Ryser}'s conjecture},
383
+ year = {2021},
384
+ eprint = {2009.07239},
385
+ archivePrefix = {arXiv},
386
+ primaryClass = {math.CO},
387
+ note = {Version 3, 3 November 2021},
388
+ howpublished = {\href{https://arxiv.org/abs/2009.07239v3}{arXiv:2009.07239v3}},
389
+ url = {https://arxiv.org/abs/2009.07239v3}
390
+ }
preprints/A-Counterexample-to-Rysers-Covering-Conjecture-September-23-2026/build/selection.tex ADDED
@@ -0,0 +1,538 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Selecting compatible translates}\label{sec:selection}
2
+
3
+ The deletion estimates require independent random choices, while
4
+ intersection of the exceptional edges requires geometric compatibility.
5
+ We separate these tasks by sampling several independent translates of
6
+ each bounded configuration and then selecting one from each pool.
7
+ The theorem below supplies the selection step. Its input consists of
8
+ finite point sets $W_i$ and sets $D_i$ of forbidden join directions;
9
+ its output avoids every forbidden join between different selected sets.
10
+ Because a direction is a linear subspace containing zero, the condition
11
+ also rules out a common point between two selected configurations
12
+ whenever at least one of their direction sets is nonempty.
13
+
14
+ \begin{theorem}[Compatible translates from independent pools]\label{thm:selection}
15
+ For every positive integer $D$ there is a positive integer $K=K(D)$
16
+ with the following property. Let $q$ tend to infinity through prime
17
+ powers. For each $q$, let $n\le Dq$, and for $1\le i\le n$ let
18
+ $W_i\subseteq\F_q^2$ and let $D_i$ be a set of directions, with
19
+ \[
20
+ |W_i|\le D,\qquad |D_i|\le D.
21
+ \]
22
+ Assume that each direction belongs to $D_i$ for at most $D$ indices $i$.
23
+ For distinct indices $i,j$, declare the translates $b+W_i$ and
24
+ $b'+W_j$ to conflict if there are $u\in W_i$, $v\in W_j$, and
25
+ $d\in D_i\cup D_j$ such that
26
+ \[
27
+ (b+u)-(b'+v)\in d.
28
+ \]
29
+ For each $i$, draw $K$ independent uniform shifts
30
+ $b_{i,1},\ldots,b_{i,K}\in\F_q^2$, independently for all indices.
31
+ With probability tending to one, one can choose $k_i\in\{1,\ldots,K\}$
32
+ for every $i$ so that the translates $b_{i,k_i}+W_i$ have no conflicts.
33
+ The convergence is uniform over all data satisfying the stated bounds.
34
+ \end{theorem}
35
+
36
+ To prove the theorem, make each candidate a vertex of a graph and
37
+ join candidates from different pools when they conflict. We seek an
38
+ independent set containing one vertex from each pool, called an
39
+ independent transversal. Its nonexistence has a small domination
40
+ certificate. We first prove the form of that assertion we need, then
41
+ show that the independent shifts make every such certificate unlikely.
42
+ The certificate argument is a weaker form of Haxell's
43
+ independent-transversal domination theorem~\cite{Haxell2001},
44
+ whose method originates in~\cite{Haxell1995}. We include its proof.
45
+ Haxell's theorem uses total domination, which also requires neighbors
46
+ for the vertices of the dominating set. Here we use the following
47
+ weaker convention.
48
+ For a graph $G$ and a set $S$ of its vertices, we say that $T\subseteq S$
49
+ \emph{dominates $S$} if every vertex of $S\setminus T$ has a neighbor in
50
+ $T$. No condition is imposed on the vertices of $T$ themselves.
51
+
52
+ \begin{lemma}[A domination certificate]\label{sel-domination}
53
+ Let a finite simple graph have a vertex partition into nonempty parts
54
+ $A_1,\ldots,A_n$. If there is no independent set containing one
55
+ vertex from each part, then there are a nonempty index set $I$ and a set
56
+ \[
57
+ T\subseteq\bigcup_{i\in I}A_i,
58
+ \qquad |T|\le 2(|I|-1),
59
+ \]
60
+ such that $T$ dominates $\bigcup_{i\in I}A_i$.
61
+ \end{lemma}
62
+
63
+ \begin{proof}
64
+ We grow a set of vertices with small size compared with the number
65
+ of parts it reaches. Whenever it does not yet dominate those parts,
66
+ we use an undominated vertex to reach another part. A minimality
67
+ condition on the transversals prevents this growth from stopping
68
+ without the required domination certificate.
69
+
70
+ Choose an inclusion-minimal nonempty subfamily of parts with no
71
+ independent transversal, and distinguish one part $A_*$ of this
72
+ subfamily. Let $\mathcal U$ be the family of independent transversals of
73
+ all its other parts. Minimality makes $\mathcal U$ nonempty. The
74
+ deficient subfamily has at least two parts, since every part is nonempty.
75
+
76
+ Choose any $x_1\in A_*$. Among $U\in\mathcal U$, minimize
77
+ $|N(x_1)\cap U|$, where $N(x)$ denotes the neighborhood of $x$ in $G$.
78
+ Fix a minimizer and write $Y_1=N(x_1)\cap U$. This set is nonempty:
79
+ otherwise adjoining $x_1$ would give an independent transversal of the
80
+ deficient subfamily.
81
+
82
+ Inductively, suppose that vertices $x_1,\ldots,x_j$ and sets
83
+ $Y_1,\ldots,Y_j$ have been fixed with the following properties:
84
+ \begin{enumerate}
85
+ \item The sets $Y_a$ are nonempty and pairwise disjoint, and some
86
+ $U\in\mathcal U$ jointly realizes all the equalities
87
+ \[
88
+ N(x_a)\cap U=Y_a\qquad(1\le a\le j).
89
+ \]
90
+ \item At stage $a$, the size $|Y_a|$ was minimized over all
91
+ $U\in\mathcal U$ satisfying the already fixed equalities for indices
92
+ smaller than $a$.
93
+ \item Each $x_a$ lies either in $A_*$ or in a part represented by a
94
+ vertex of some earlier $Y_b$, with $b<a$.
95
+ \end{enumerate}
96
+ Let $Y=\bigcup_{a=1}^jY_a$, let $I$ consist of the distinguished part
97
+ and all parts represented in $Y$, and put
98
+ \[
99
+ T=\{x_1,\ldots,x_j\}\cup Y.
100
+ \]
101
+ By joint realization, the vertices of $Y$ occupy distinct parts, none
102
+ of them $A_*$. Thus $|I|=|Y|+1$, while nonemptiness of the $Y_a$ gives
103
+ $j\le |Y|$. The third invariant shows that $T$ lies in the union of
104
+ the parts indexed by $I$, and
105
+ \[
106
+ |T|\le j+|Y|\le 2|Y|=2(|I|-1).
107
+ \]
108
+ If $T$ dominates this union, we have the required certificate.
109
+
110
+ Otherwise, choose a vertex $x_{j+1}$ in that union, outside $T$, with
111
+ no neighbor in $T$. Among the transversals realizing all the current
112
+ equalities, choose $U$ minimizing $|N(x_{j+1})\cap U|$, and set
113
+ \[
114
+ Y_{j+1}=N(x_{j+1})\cap U.
115
+ \]
116
+ This set avoids all the previous $Y_a$, because $x_{j+1}$ has no
117
+ neighbor in $T$. We claim it is nonempty.
118
+
119
+ If it were empty and $x_{j+1}\in A_*$, then $U\cup\{x_{j+1}\}$
120
+ would be an independent transversal of the deficient subfamily.
121
+ Otherwise, the part of $x_{j+1}$ contains a unique vertex $y$ of $Y$,
122
+ say $y\in Y_b$. The transversal $U$ uses $y$ in that part, so
123
+ $x_{j+1}\notin U$. Replace $y$ by $x_{j+1}$ to form
124
+ \[
125
+ U'=(U\setminus\{y\})\cup\{x_{j+1}\}.
126
+ \]
127
+ Since $N(x_{j+1})\cap U=\varnothing$, this is again an independent
128
+ transversal of the nondistinguished parts. For every $a<b$, the vertex
129
+ $y$ does not belong to $Y_a$, and the new vertex is not adjacent to
130
+ $x_a$. Consequently the exact earlier equalities are preserved:
131
+ \[
132
+ N(x_a)\cap U'=Y_a\qquad(a<b).
133
+ \]
134
+ For $a=b$, the replacement removes the neighbor $y$ and adds no neighbor,
135
+ so
136
+ \[
137
+ |N(x_b)\cap U'|=|Y_b|-1.
138
+ \]
139
+ This contradicts the minimum imposed at stage $b$. Notice that the
140
+ contradiction uses only the equalities preceding stage $b$; preservation
141
+ of later equalities is not required.
142
+
143
+ Thus $Y_{j+1}$ is nonempty and all the induction invariants continue to
144
+ hold. Each continuation adds vertices in previously unrepresented
145
+ parts to $Y$, whereas all of $Y$ lies in one transversal of the fixed
146
+ nondistinguished subfamily. There can be only finitely many
147
+ continuations. The process must therefore stop with a dominating set
148
+ $T$, proving the lemma.
149
+ \end{proof}
150
+
151
+ \begin{proof}[Proof of Theorem~\ref{thm:selection}]
152
+ The case $n=0$ is immediate, so suppose $n\ge1$. Fix $D$ and, for the
153
+ moment, a constant integer $K\ge6$. We will choose $K$ sufficiently
154
+ large in terms of $D$ at the end.
155
+
156
+ Form a graph whose vertices are the candidate positions $(i,k)$,
157
+ partitioned into the $n$ pools. Put an edge between candidates in
158
+ different pools precisely when their translates conflict. Candidate
159
+ positions are distinct vertices even when their sampled shifts happen
160
+ to coincide. An independent transversal in this graph is exactly a
161
+ selection as in the theorem.
162
+
163
+ By Lemma~\ref{sel-domination}, it suffices to show that, with probability
164
+ tending to one, there are no nonempty index sets $I$, with $|I|=m$, and
165
+ sets $T$ of at most $2m$ candidate positions in those pools that dominate
166
+ their union. We use the slightly weaker bound $2m$ to simplify the
167
+ counting. Throughout the probability estimates, $I$ and $T$ are fixed
168
+ sets of indices before any shifts are exposed.
169
+
170
+ The proof splits according to $m$, the number of pools in the
171
+ certificate. When $m$ is small, the forbidden lines associated with
172
+ $T$ occupy only a small part of each candidate's possible shifts.
173
+ When $m$ is proportional to $q$, that direct bound is insufficient.
174
+ Instead, we expose $T$ in a bounded number of chunks and prove that
175
+ a positive average proportion of shifts remains feasible. Crucially,
176
+ this proportion will depend only on $D$, so we may subsequently choose
177
+ $K$ large enough that the unused candidates defeat all certificates.
178
+
179
+ \paragraph{Forbidden equations and counting possible certificates.}
180
+ For every direction $d$ in use, fix a nonzero linear functional
181
+ $\pi_d:\F_q^2\to\F_q$ whose kernel is $d$. After exposing the shifts
182
+ of the candidates $e\in T$, call a shift $b\in\F_q^2$ \emph{feasible
183
+ for target $i$} if, for every such $e$, with source-pool index $j$, it
184
+ avoids every equation
185
+ \begin{equation}\label{sel-forbidden}
186
+ \pi_d(b)=\pi_d(b_e)+\pi_d(v-u),
187
+ \qquad
188
+ u\in W_i,\quad v\in W_j,\quad d\in D_i\cup D_j.
189
+ \end{equation}
190
+ We impose these prohibitions even when $i=j$. This only makes
191
+ feasibility more restrictive. A feasible candidate outside $T$ has no
192
+ neighbor in $T$, so its existence prevents domination.
193
+
194
+ Set
195
+ \begin{equation}\label{sel-constants}
196
+ C=2D^3,\qquad c_1=\frac1{4C},\qquad \alpha=\frac1{2C}.
197
+ \end{equation}
198
+ For one target $i$ and one exposed candidate $e$, there are at most $C$
199
+ equations in \eqref{sel-forbidden}. This remains true if the two lists
200
+ $D_i$ and $D_j$ are counted separately, retaining duplicate directions.
201
+ Each equation excludes one affine line, containing exactly $q$ shifts.
202
+
203
+ The number of choices of $I$ is at most
204
+ \[
205
+ \binom{n}{m}\le\left(\frac{eDq}{m}\right)^m.
206
+ \]
207
+ There is an absolute constant $C_*>0$ such that, for $K\ge6$, the number
208
+ of candidate-index sets $T$ in these pools with $|T|\le2m$ is at most
209
+ \begin{equation}\label{sel-certificate-count}
210
+ \sum_{t=0}^{2m}\binom{Km}{t}\le (C_*K^2)^m.
211
+ \end{equation}
212
+ For example, the usual bound
213
+ $\sum_{t=0}^{r}\binom Nt\le(eN/r)^r$ for $1\le r\le N/2$
214
+ applies with $N=Km$ and $r=2m$.
215
+
216
+ \paragraph{The range $1\le m\le c_1q$.}
217
+ Condition on all the exposed shifts in $T$. A fresh uniform shift for
218
+ any target $i\in I$ is infeasible with probability at most
219
+ \[
220
+ \frac{C|T|}{q}\le\frac{2Cm}{q}\le\frac12.
221
+ \]
222
+ At least $(K-2)m$ candidate positions in the target pools remain
223
+ unexposed. Their shifts are conditionally independent and uniform.
224
+ Thus the probability that $T$ dominates, for this fixed $I,T$, is at most
225
+ \begin{equation}\label{sel-small-probability}
226
+ \left(\frac{2Cm}{q}\right)^{(K-2)m}.
227
+ \end{equation}
228
+ Combining this with the counts of $I$ and $T$, the probability of a
229
+ dominating certificate of size parameter $m$ is at most
230
+ \begin{equation}\label{sel-small-sum}
231
+ \left[
232
+ 2CeD C_*K^2
233
+ \left(\frac{2Cm}{q}\right)^{K-3}
234
+ \right]^m.
235
+ \end{equation}
236
+ Choose $K$ large enough that
237
+ \begin{equation}\label{sel-small-K}
238
+ 2CeD C_*K^2\,2^{-(K-3)}\le\frac12.
239
+ \end{equation}
240
+ Then the bracket in \eqref{sel-small-sum} is at most $1/2$ throughout
241
+ this range, and tends to zero for every fixed positive $m$. Summing
242
+ over $m$ gives $o(1)$: for a fixed cutoff, the finite initial sum tends
243
+ to zero, while the remaining terms are bounded by a geometric tail.
244
+
245
+ \paragraph{A feasible-density estimate for $m>c_1q$.}
246
+ We prove that there is a constant $\delta_1>0$, depending only on $D$
247
+ and not on $K$, such that for every fixed $I,T$ in this range,
248
+ \begin{equation}\label{sel-density-target}
249
+ \Pr\!\left[
250
+ \sum_{i\in I}|U_i^{\mathrm{fin}}|<\delta_1mq^2
251
+ \right]
252
+ \le \exp\bigl(-\Omega_D(q\log q)\bigr).
253
+ \end{equation}
254
+ Here $U_i^{\mathrm{fin}}$ is the set of shifts feasible for target $i$
255
+ after all candidates in $T$ have been exposed. The estimate is uniform
256
+ in $I,T$ and the configuration data. The lower cutoff on $q$ may
257
+ depend on the fixed value of $K$.
258
+
259
+ Expose the candidate positions of $T$ in a fixed order, divided into
260
+ consecutive chunks of size at most $\lfloor\alpha q\rfloor$, with all
261
+ but the last having that size. For sufficiently large $q$,
262
+ $\lfloor\alpha q\rfloor\ge\alpha q/2$. Since $|T|\le2m\le2Dq$,
263
+ the number of chunks is at most
264
+ \begin{equation}\label{sel-chunk-count}
265
+ J_0=\left\lceil\frac{4D}{\alpha}+1\right\rceil.
266
+ \end{equation}
267
+ In particular, this bound does not involve $K$. If $T$ is empty, the
268
+ desired feasible-density estimate holds deterministically; otherwise
269
+ there is at least one chunk.
270
+
271
+ At the start of a chunk, condition on all shifts previously exposed.
272
+ Let $U_i$ be the set of shifts still feasible for target $i$, and write
273
+ \[
274
+ M=\sum_{i\in I}|U_i|.
275
+ \]
276
+ For the analysis of this chunk we keep all these sets frozen at their
277
+ start values. They are now deterministic, while the shifts belonging
278
+ to the new chunk are independent uniform vectors.
279
+
280
+ For an entry $e$ of the chunk, with source-pool index $j$, define $Z_e$
281
+ by summing, over all equations \eqref{sel-forbidden} associated with
282
+ $i\in I$ and $e$, the number of shifts $b\in U_i$ satisfying that
283
+ equation. Count the $D_i$ and $D_j$ lists separately, including
284
+ duplicates. A shift deleted more than once is therefore counted more
285
+ than once, which is harmless for an upper bound on loss. Each line
286
+ contains at most $q$ shifts, and each of its right-hand sides is uniform
287
+ in $\F_q$. Consequently,
288
+ \begin{equation}\label{sel-Z-basic}
289
+ 0\le Z_e\le Cmq,
290
+ \qquad \E Z_e\le \frac{CM}{q}.
291
+ \end{equation}
292
+ All expectations and variances in the following chunk calculation are
293
+ conditional on the fixed past.
294
+
295
+ \paragraph{The terms whose directions belong to the target.}
296
+ The expectation bound alone does not control the loss in a chunk.
297
+ We estimate its fluctuations by separating the two direction lists
298
+ in each forbidden equation. Bounded reuse of target directions handles
299
+ one list; the affine second moment will handle the source list.
300
+ Write
301
+ \[
302
+ Z_e=Z_e^{(1)}+Z_e^{(2)},
303
+ \]
304
+ where $Z_e^{(1)}$ uses the list $D_i$ in each target, and $Z_e^{(2)}$
305
+ uses the list $D_j$ of the source. Group the terms of $Z_e^{(1)}$ by
306
+ direction. The group for $d$ is a function only of $\pi_d(b_e)$.
307
+ For distinct directions $d,d'$, the functionals $\pi_d,\pi_{d'}$ are
308
+ linearly independent, so
309
+ \[
310
+ b_e\longmapsto\bigl(\pi_d(b_e),\pi_{d'}(b_e)\bigr)
311
+ \]
312
+ is a bijection from $\F_q^2$ to itself. The two coordinates are
313
+ therefore independent and uniform. The direction groups are pairwise
314
+ independent, which suffices for adding their variances.
315
+
316
+ There are at most $Dm$ such groups. Each direction belongs to at most
317
+ $D$ target direction sets; for each associated target-source pair
318
+ there are at most $D^2$ choices of $(u,v)$. Thus every group is bounded
319
+ by $D^3q$, and
320
+ \begin{equation}\label{sel-first-variance}
321
+ \operatorname{Var}(Z_e^{(1)})\le D^7mq^2.
322
+ \end{equation}
323
+
324
+ \paragraph{The terms whose directions belong to the source.}
325
+ For each target $i$ and each direction $d$, define the variance of its
326
+ parallel line slices by
327
+ \begin{equation}\label{sel-slice-variance}
328
+ V_{i,d}=\frac1q\sum_{\ell\parallel d}
329
+ \left(|U_i\cap\ell|-\frac{|U_i|}{q}\right)^2,
330
+ \end{equation}
331
+ where the sum is over the $q$ affine lines of direction $d$.
332
+ These variances obey the exact identity
333
+ \begin{equation}\label{sel-energy}
334
+ \sum_d V_{i,d}
335
+ =|U_i|-\frac{|U_i|^2}{q^2}
336
+ \le |U_i|\le q^2,
337
+ \end{equation}
338
+ where the sum runs over all $q+1$ directions. This is precisely the
339
+ normalized affine second-moment identity
340
+ in~\cite[Lemma~A.1]{OpenAI2026Balanced}, applied to $U_i\subseteq\F_q^2$.
341
+ That identity holds for every subset of every finite affine plane;
342
+ it has no randomness, characteristic, or subfield hypothesis. Thus it
343
+ applies after conditioning on any history of earlier chunks. This is
344
+ the reason we can control all source directions even when the feasible
345
+ sets $U_i$ have complicated shapes.
346
+
347
+ Every individual summand of $Z_e^{(2)}$ associated with $i,d,u,v$ is a
348
+ uniformly sampled line-slice count, with its slice index translated by
349
+ a fixed offset. Its variance is therefore $V_{i,d}$. There are at
350
+ most $D^3m$ summands, and each pair $(i,d)$ is repeated at most $D^2$
351
+ times. Cauchy--Schwarz applied to their centered sum, without any
352
+ independence assumption, gives
353
+ \begin{equation}\label{sel-second-variance}
354
+ \operatorname{Var}(Z_e^{(2)})
355
+ \le D^5m A_e,
356
+ \qquad
357
+ A_e:=\sum_{i\in I}\sum_{d\in D_j}V_{i,d}.
358
+ \end{equation}
359
+
360
+ Each source pool contributes at most $K$ entries to the chunk, and
361
+ each direction belongs to at most $D$ source direction sets.
362
+ Consequently, by \eqref{sel-energy},
363
+ \begin{equation}\label{sel-exception-energy}
364
+ \sum_{e\text{ in the chunk}} A_e
365
+ \le KD\sum_{i\in I}\sum_d V_{i,d}
366
+ \le KDmq^2.
367
+ \end{equation}
368
+ Call an entry \emph{regular} if $A_e\le mq^{3/2}$. There are at most
369
+ $KD\sqrt q$ irregular entries. For a regular entry,
370
+ \eqref{sel-first-variance}, \eqref{sel-second-variance}, and
371
+ $\operatorname{Var}(X+Y)\le2\operatorname{Var}(X)+2\operatorname{Var}(Y)$
372
+ give
373
+ \begin{equation}\label{sel-regular-variance}
374
+ \operatorname{Var}(Z_e)
375
+ \le 2D^7mq^2+2D^5m^2q^{3/2}.
376
+ \end{equation}
377
+ For a fixed constant $\gamma>0$, Chebyshev's inequality and
378
+ \eqref{sel-Z-basic} therefore imply
379
+ \begin{align}
380
+ \Pr\!\left[Z_e>\frac{CM}{q}+\gamma mq\right]
381
+ &\le \frac{2D^7}{\gamma^2m}
382
+ +\frac{2D^5}{\gamma^2\sqrt q}
383
+ \notag\\
384
+ &\le B_{D,\gamma}q^{-1/2}
385
+ \qquad\text{for regular }e,
386
+ \label{sel-regular-tail}
387
+ \end{align}
388
+ where $B_{D,\gamma}$ is independent of $K$. In the last step we used
389
+ $m>c_1q$.
390
+
391
+ \paragraph{Conditional independence and loss over one chunk.}
392
+ The preceding variance bounds show that each regular entry has a
393
+ small chance of removing far more than its expected share. We now
394
+ use independence within the chunk to show that few entries do so,
395
+ and convert that statement into a deterministic bound on the total
396
+ remaining feasible set.
397
+
398
+ The regularity of an entry is determined by the frozen sets $U_i$ and
399
+ its fixed source-pool index. In particular, it does not depend on its
400
+ fresh shift $b_e$. After conditioning on the past, the collection of
401
+ regular entries is fixed, and their variables $Z_e$ are independent
402
+ functions of independent shifts. Their common threshold in
403
+ \eqref{sel-regular-tail} is also fixed under this conditioning.
404
+
405
+ A union bound over subsets of regular entries, using the chunk size
406
+ bound and \eqref{sel-regular-tail}, shows that the probability of at
407
+ least $\gamma q$ threshold exceedances is at most
408
+ \begin{equation}\label{sel-chunk-tail}
409
+ 2^{\lceil\alpha q\rceil}
410
+ \left(B_{D,\gamma}q^{-1/2}\right)^{\lceil\gamma q\rceil}
411
+ \le \exp(-c_{D,\gamma}q\log q)
412
+ \end{equation}
413
+ for all sufficiently large $q$, with $c_{D,\gamma}>0$ independent of
414
+ $K$. If there are fewer than $\lceil\gamma q\rceil$ regular entries,
415
+ the event in question is empty and the bound remains valid.
416
+
417
+ For each fixed $K$, we may also take $q$ sufficiently large that
418
+ \begin{equation}\label{sel-K-cutoff}
419
+ KD\sqrt q\le\gamma q.
420
+ \end{equation}
421
+ Except on the event in \eqref{sel-chunk-tail}, all but at most
422
+ $2\gamma q$ entries are regular and below the threshold: the exceptions
423
+ include all irregular entries. The actual loss of feasible shifts
424
+ within the chunk is at most $\sum_eZ_e$, because these counts used the
425
+ larger feasible sets at the start of the chunk. Bounding each
426
+ exceptional entry by $Cmq$ and all other entries by the threshold gives,
427
+ for the end-of-chunk value $M'$, the deterministic inequality
428
+ \begin{align}
429
+ M'
430
+ &\ge M-C\alpha M-\alpha\gamma mq^2-2C\gamma mq^2
431
+ \notag\\
432
+ &=(1-C\alpha)M-(\alpha+2C)\gamma mq^2
433
+ \notag\\
434
+ &=\frac12M-(\alpha+2C)\gamma mq^2.
435
+ \label{sel-chunk-recurrence}
436
+ \end{align}
437
+
438
+ Choose $\gamma>0$, depending only on $D$, so small that
439
+ \begin{equation}\label{sel-gamma-choice}
440
+ 2(\alpha+2C)\gamma\le 2^{-J_0-1},
441
+ \qquad
442
+ \delta_1:=2^{-J_0-1}.
443
+ \end{equation}
444
+ At the beginning, before exposing $T$, every shift is feasible, so
445
+ $M=mq^2$. If all $J\le J_0$ chunks satisfy
446
+ \eqref{sel-chunk-recurrence}, iteration gives
447
+ \begin{align*}
448
+ \frac{M_{\mathrm{fin}}}{mq^2}
449
+ &\ge 2^{-J}-(\alpha+2C)\gamma
450
+ \sum_{a=0}^{J-1}2^{-a}\\
451
+ &\ge 2^{-J_0}-2(\alpha+2C)\gamma
452
+ \ge\delta_1.
453
+ \end{align*}
454
+ The conditional probability bound \eqref{sel-chunk-tail} holds for
455
+ every possible past. Averaging over the past and taking a union bound
456
+ over the at most $J_0$ chunks proves \eqref{sel-density-target}.
457
+ The constants $J_0$, $\gamma$, and $\delta_1$ depend only on $D$.
458
+ The dependence on $K$ in \eqref{sel-K-cutoff} affects only how large
459
+ $q$ must be, not these constants.
460
+
461
+ \paragraph{Unused candidates and the large-range union bound.}
462
+ We have established the required positive average feasible density
463
+ with a failure probability of order $\exp(-\Omega_D(q\log q))$.
464
+ There are only exponentially many candidate certificates, so this
465
+ error can be summed over all of them. On the successful event, the
466
+ unused candidates now supply the further exponential saving needed
467
+ to rule out domination.
468
+
469
+ Condition now on all the shifts belonging to $T$, and suppose the
470
+ feasible-density event in \eqref{sel-density-target} succeeds. Let
471
+ $t_i$ be the number of exposed candidate positions from pool $i$.
472
+ Every unused candidate from that pool remains independent and uniform,
473
+ and is feasible with probability $|U_i^{\mathrm{fin}}|/q^2$.
474
+ The probability that none of the unused candidates in the target pools
475
+ is feasible is therefore at most
476
+ \begin{align}
477
+ \prod_{i\in I}
478
+ \left(1-\frac{|U_i^{\mathrm{fin}}|}{q^2}\right)^{K-t_i}
479
+ &\le
480
+ \exp\!\left(-\sum_{i\in I}
481
+ (K-t_i)\frac{|U_i^{\mathrm{fin}}|}{q^2}\right)
482
+ \notag\\
483
+ &\le \exp\bigl(-(K\delta_1-2)m\bigr).
484
+ \label{sel-unused-candidates}
485
+ \end{align}
486
+ To obtain the last inequality, use
487
+ \[
488
+ \sum_{i\in I}\frac{|U_i^{\mathrm{fin}}|}{q^2}\ge\delta_1m,
489
+ \qquad
490
+ 0\le\frac{|U_i^{\mathrm{fin}}|}{q^2}\le1,
491
+ \qquad
492
+ \sum_{i\in I}t_i=|T|\le2m.
493
+ \]
494
+ This argument also covers pools for which every candidate belongs to
495
+ $T$; it does not assume $K-t_i$ is positive in every target pool.
496
+
497
+ For $m>c_1q$, the number of pairs $I,T$ is at most $A_K^m$, where
498
+ \begin{equation}\label{sel-large-count}
499
+ A_K=\frac{eD}{c_1}C_*K^2.
500
+ \end{equation}
501
+ For each fixed pair, domination can occur only if the feasible-density
502
+ estimate fails or all unused candidates are infeasible despite its
503
+ success. The sum of the first failure probabilities over all
504
+ $m,I,T$ in the large range is bounded by
505
+ \[
506
+ \exp\bigl(O_{D,K}(q)\bigr)
507
+ \exp\bigl(-\Omega_D(q\log q)\bigr)=o(1).
508
+ \]
509
+ Here the number of choices is at most
510
+ $\sum_{m\le Dq}A_K^m=\exp(O_{D,K}(q))$, with $K$ fixed.
511
+
512
+ Finally choose $K$ sufficiently large, still depending only on $D$, so
513
+ that both \eqref{sel-small-K} and
514
+ \begin{equation}\label{sel-large-K}
515
+ A_K\exp(2-K\delta_1)<\frac12
516
+ \end{equation}
517
+ hold. Such a choice exists because $\delta_1>0$ does not depend on $K$,
518
+ whereas $A_K$ grows only quadratically in $K$. By
519
+ \eqref{sel-unused-candidates}, the sum of the remaining failure
520
+ probabilities is then at most
521
+ \[
522
+ \sum_{m>c_1q}
523
+ \left(A_K\exp(2-K\delta_1)\right)^m
524
+ \le\sum_{m>c_1q}2^{-m}=o(1).
525
+ \]
526
+ Together with the small-range estimate, this excludes all dominating
527
+ certificates with probability tending to one. Lemma~\ref{sel-domination}
528
+ therefore supplies an independent transversal, proving the theorem.
529
+
530
+ The choices have been made in the order
531
+ \[
532
+ D\ ;\quad C,c_1,\alpha,J_0,\gamma,\delta_1\ ;\quad K\ ;\quad q.
533
+ \]
534
+ In particular, $K$ is fixed before taking $q$ to infinity, and all
535
+ sufficiently-large-$q$ conditions may depend on that fixed $K$.
536
+ Every estimate above is uniform over the configurations and direction
537
+ sets subject to the bounds in the theorem.
538
+ \end{proof}
preprints/A-Counterexample-to-Rysers-Covering-Conjecture-September-23-2026/paper.pdf ADDED
@@ -0,0 +1,3 @@
 
 
 
 
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preprints/A-Counterexample-to-Walls-D2-Problem-October-6-2026/README.md ADDED
@@ -0,0 +1,18 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ # [A Counterexample to Wall's D(2) Problem](wall-d2-counterexample.pdf)
2
+
3
+ **Author:** OpenAI
4
+
5
+ **Date:** October 6, 2026
6
+
7
+ ## Citation
8
+
9
+ ```bibtex
10
+ @misc{OAI:A-Counterexample-to-Walls-D2-Problem-October-6-2026,
11
+ author = {{OpenAI}},
12
+ title = {{A Counterexample to Wall's $D(2)$ Problem}},
13
+ howpublished = {OpenAI Math Release preprint
14
+ \href{https://github.com/openai/math/blob/main/preprints/A-Counterexample-to-Walls-D2-Problem-October-6-2026/wall-d2-counterexample.pdf}{OAI:A-Counterexample-to-Walls-D2-Problem-October-6-2026}},
15
+ year = {2026}
16
+ }
17
+ ```
18
+
preprints/A-Counterexample-to-Walls-D2-Problem-October-6-2026/build/figures/tower.tex ADDED
@@ -0,0 +1,20 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \begin{tikzpicture}[
2
+ >=Latex,
3
+ every node/.style={font=\normalsize},
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+ every edge/.style={draw,->,semithick},
5
+ baseline=(current bounding box.center)
6
+ ]
7
+ \node (F) at (0,0) {$F$};
8
+ \node (next) at (3,1.1) {$A_{i+1}$};
9
+ \node (cover) at (6.2,1.1) {$\widehat A_i$};
10
+ \node (base) at (6.2,-1.1) {$A_i$};
11
+ \path (F) edge node[above,sloped] {$f_{i+1}$} (next);
12
+ \draw[semithick,{Hooks[right]}-Latex]
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+ (next) -- node[above] {inclusion} (cover);
14
+ \path (cover) edge node[right] {$p_i$} (base);
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+ \node[anchor=west,font=\small,align=left] at (6.85,0)
16
+ {infinite cyclic\\cover};
17
+ \path (F) edge node[below,sloped] {$f_i$} (base);
18
+ \node[font=\small] at (2.85,-1.85)
19
+ {$s(A_i)<s(A_{i+1})\leq s(F)$};
20
+ \end{tikzpicture}
preprints/A-Counterexample-to-Walls-D2-Problem-October-6-2026/build/main.tex ADDED
@@ -0,0 +1,20 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \documentclass[11pt]{article}
2
+ \input{preamble}
3
+ \title{A Counterexample to Wall's \texorpdfstring{$D(2)$}{D(2)} Problem}
4
+ \author{OpenAI}
5
+ \date{October 6, 2026}
6
+ \begin{document}
7
+ \maketitle
8
+ \begin{abstract}
9
+ We give a negative answer to Wall's finite $D(2)$ problem. We construct
10
+ a finite connected three-dimensional CW complex satisfying the $D(2)$
11
+ finiteness condition but not homotopy equivalent to any finite CW complex
12
+ of dimension at most two. The example has infinite fundamental group.
13
+ \end{abstract}
14
+ \input{sections/01-introduction}
15
+ \input{sections/02-tower}
16
+ \input{sections/03-plus}
17
+ \input{sections/04-construction}
18
+ \bibliographystyle{alpha}
19
+ \bibliography{references}
20
+ \end{document}
preprints/A-Counterexample-to-Walls-D2-Problem-October-6-2026/build/preamble.tex ADDED
@@ -0,0 +1,27 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
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+ \usepackage[T1]{fontenc}
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+ \usepackage{lmodern}
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+ \usepackage[margin=1in]{geometry}
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+ \usepackage{amsmath,amssymb,amsthm,mathtools}
5
+ \usepackage{microtype,enumitem,needspace,placeins,xcolor,tikz,booktabs}
6
+ \usetikzlibrary{arrows.meta,positioning,calc}
7
+ \usepackage[colorlinks=true,linkcolor=blue!45!black,citecolor=blue!45!black,urlcolor=blue!45!black]{hyperref}
8
+ \hypersetup{pdftitle={A Counterexample to Wall's D(2) Problem},pdfauthor={OpenAI}}
9
+ \newtheorem{theorem}{Theorem}[section]
10
+ \newtheorem{proposition}[theorem]{Proposition}
11
+ \newtheorem{lemma}[theorem]{Lemma}
12
+ \newtheorem{corollary}[theorem]{Corollary}
13
+ \theoremstyle{definition}
14
+ \newtheorem{definition}[theorem]{Definition}
15
+ \newtheorem{remark}[theorem]{Remark}
16
+ \newcommand{\C}{\mathbb C}
17
+ \newcommand{\Z}{\mathbb Z}
18
+ \newcommand{\Q}{\mathbb Q}
19
+ \newcommand{\RP}{\mathbb{RP}}
20
+ \newcommand{\Hom}{\operatorname{Hom}}
21
+ \newcommand{\id}{\operatorname{id}}
22
+ \newcommand{\im}{\operatorname{im}}
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+ \newcommand{\ab}{\mathrm{ab}}
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+ \newcommand{\rk}{\operatorname{rank}}
25
+ \setlist[enumerate]{label=\textup{(\roman*)},leftmargin=*}
26
+ \setlength{\emergencystretch}{1.5em}
27
+ \allowdisplaybreaks[1]
preprints/A-Counterexample-to-Walls-D2-Problem-October-6-2026/build/references.bib ADDED
@@ -0,0 +1,148 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ @article{Wall65,
2
+ author = {Wall, C. T. C.},
3
+ title = {Finiteness conditions for {CW}-complexes},
4
+ journal = {Annals of Mathematics. Second Series},
5
+ volume = {81},
6
+ number = {1},
7
+ year = {1965},
8
+ pages = {56--69},
9
+ doi = {10.2307/1970382}
10
+ }
11
+
12
+ @incollection{Wall79,
13
+ author = {Wall, C. T. C.},
14
+ title = {List of problems},
15
+ booktitle = {Homological Group Theory},
16
+ editor = {Wall, C. T. C.},
17
+ series = {London Mathematical Society Lecture Note Series},
18
+ volume = {36},
19
+ publisher = {Cambridge University Press},
20
+ address = {Cambridge},
21
+ year = {1979},
22
+ pages = {369--394}
23
+ }
24
+
25
+ @book{Johnson03,
26
+ author = {Johnson, F. E. A.},
27
+ title = {Stable Modules and the {D(2)}-Problem},
28
+ series = {London Mathematical Society Lecture Note Series},
29
+ volume = {301},
30
+ publisher = {Cambridge University Press},
31
+ address = {Cambridge},
32
+ year = {2003},
33
+ doi = {10.1017/CBO9780511550256}
34
+ }
35
+
36
+ @incollection{Cohen78,
37
+ author = {Cohen, J. M.},
38
+ title = {Complexes of cohomological dimension two},
39
+ booktitle = {Algebraic and Geometric Topology},
40
+ series = {Proceedings of Symposia in Pure Mathematics},
41
+ volume = {32},
42
+ publisher = {American Mathematical Society},
43
+ address = {Providence, RI},
44
+ year = {1978},
45
+ pages = {221--223},
46
+ note = {Part 2}
47
+ }
48
+
49
+ @article{Hambleton18,
50
+ author = {Hambleton, Ian},
51
+ title = {Two remarks on {Wall's D2} problem},
52
+ journal = {Mathematical Proceedings of the Cambridge Philosophical Society},
53
+ volume = {167},
54
+ year = {2019},
55
+ pages = {361--368}
56
+ }
57
+
58
+ @article{HofmannNicholson27,
59
+ author = {Hofmann, Tommy and Nicholson, John},
60
+ title = {Exotic presentations of quaternion groups and {Wall's D2} problem},
61
+ journal = {Journal of Algebra},
62
+ volume = {712},
63
+ year = {2027},
64
+ pages = {253--310},
65
+ doi = {10.1016/j.jalgebra.2026.06.040}
66
+ }
67
+
68
+ @article{Mannan09,
69
+ author = {Mannan, W. H.},
70
+ title = {{Quillen's} plus construction and the {D(2)} problem},
71
+ journal = {Algebraic \& Geometric Topology},
72
+ volume = {9},
73
+ number = {3},
74
+ year = {2009},
75
+ pages = {1399--1411},
76
+ doi = {10.2140/agt.2009.9.1399}
77
+ }
78
+
79
+ @article{Fox53,
80
+ author = {Fox, Ralph H.},
81
+ title = {Free differential calculus. {I}. {Derivation} in the free group ring},
82
+ journal = {Annals of Mathematics. Second Series},
83
+ volume = {57},
84
+ number = {3},
85
+ year = {1953},
86
+ pages = {547--560},
87
+ doi = {10.2307/1969736}
88
+ }
89
+
90
+ @article{Howie81Pairs,
91
+ author = {Howie, James},
92
+ title = {On pairs of 2-complexes and systems of equations over groups},
93
+ journal = {Journal f\"ur die reine und angewandte Mathematik},
94
+ volume = {324},
95
+ year = {1981},
96
+ pages = {165--174},
97
+ doi = {10.1515/crll.1981.324.165}
98
+ }
99
+
100
+ @article{LouderWilton17,
101
+ author = {Louder, Larsen and Wilton, Henry},
102
+ title = {Stackings and the {W}-cycles conjecture},
103
+ journal = {Canadian Mathematical Bulletin},
104
+ volume = {60},
105
+ number = {3},
106
+ year = {2017},
107
+ pages = {604--612}
108
+ }
109
+
110
+ @incollection{Quillen71,
111
+ author = {Quillen, Daniel},
112
+ title = {Cohomology of groups},
113
+ booktitle = {Actes du Congr\`es International des Math\'ematiciens (Nice, 1970)},
114
+ volume = {2},
115
+ publisher = {Gauthier-Villars},
116
+ address = {Paris},
117
+ year = {1971},
118
+ pages = {47--51}
119
+ }
120
+
121
+ @article{BridsonTweedale07,
122
+ author = {Bridson, Martin R. and Tweedale, Michael},
123
+ title = {Deficiency and abelianized deficiency of some virtually free groups},
124
+ journal = {Mathematical Proceedings of the Cambridge Philosophical Society},
125
+ volume = {143},
126
+ year = {2007},
127
+ pages = {257--264}
128
+ }
129
+
130
+ @article{MannanPopiel21,
131
+ author = {Mannan, W. H. and Popiel, Tomasz},
132
+ title = {An exotic presentation of {$Q_{28}$}},
133
+ journal = {Algebraic \& Geometric Topology},
134
+ volume = {21},
135
+ number = {4},
136
+ year = {2021},
137
+ pages = {2065--2084}
138
+ }
139
+
140
+ @article{Nicholson21,
141
+ author = {Nicholson, John},
142
+ title = {On {CW}-complexes over groups with periodic cohomology},
143
+ journal = {Transactions of the American Mathematical Society},
144
+ volume = {374},
145
+ number = {9},
146
+ year = {2021},
147
+ pages = {6531--6557}
148
+ }
preprints/A-Counterexample-to-Walls-D2-Problem-October-6-2026/build/sections/01-introduction.tex ADDED
@@ -0,0 +1,131 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Introduction}\label{sec:introduction}
2
+
3
+ Wall's finiteness conditions ask when algebraic restrictions on a CW
4
+ complex force it to have a homotopy model of a prescribed dimension.
5
+ Let $X$ be a finite connected CW complex, let $G=\pi_1(X)$, and let
6
+ $\widetilde X$ be its universal cover. The $D(2)$ condition is
7
+ \begin{equation}\label{eq:d2-condition}
8
+ H_i(\widetilde X;\Z)=0\quad(i>2),\qquad
9
+ H^3(X;M)=0\quad\text{for every finitely generated }\Z G\text{-module }M,
10
+ \end{equation}
11
+ where cohomology uses the corresponding local coefficients.
12
+ The finite $D(2)$ problem asks whether every such $X$ is homotopy
13
+ equivalent to a finite CW complex of dimension at most two
14
+ \cite[Section~2]{Wall65}, \cite[Problem~D3]{Wall79}.
15
+ The finiteness of both complexes is part of the question, and no
16
+ asphericity hypothesis is imposed. This is also the formulation in
17
+ Hofmann--Nicholson~\cite[p.~254]{HofmannNicholson27}.
18
+
19
+ \begin{theorem}\label{thm:main}
20
+ There is a finite connected three-dimensional CW complex $X$ such that
21
+ \[
22
+ H_i(\widetilde X;\Z)=0\quad(i>2),\qquad
23
+ H^3(X;M)=0\quad\text{for every }\Z[\pi_1(X)]\text{-module }M,
24
+ \]
25
+ but $X$ is not homotopy equivalent to any finite CW complex of
26
+ dimension at most two.
27
+ \end{theorem}
28
+
29
+ The example has infinite fundamental group; the finiteness assertion
30
+ concerns its cell structure.
31
+
32
+ \subsection{Background and approach}
33
+
34
+ Wall introduced the dimension conditions in his work on finiteness
35
+ for CW complexes~\cite{Wall65}. His reduction produces a finite
36
+ three-dimensional model in the $D(2)$ case; the remaining question is
37
+ whether its three-dimensional cells can also be removed up to homotopy.
38
+ The problem reappeared as Problem~D3 in his 1979 list~\cite{Wall79}.
39
+ It lies at the interface between two-dimensional topology and the
40
+ realization of chain complexes over group rings. Johnson's work
41
+ \cite{Johnson03} develops this algebraic viewpoint and the role of
42
+ cancellation in passing from a stable realization to an actual
43
+ two-dimensional complex.
44
+
45
+ A stable form of the problem has a positive answer: adjoining
46
+ sufficiently many two-spheres makes a finite $D(2)$ complex homotopy
47
+ equivalent to a finite two-dimensional complex. This goes back to
48
+ Cohen~\cite{Cohen78}; Hambleton~\cite[Lemma~2.1]{Hambleton18} gives
49
+ a proof with the number of added spheres bounded by the number of
50
+ three-dimensional cells. Such stabilization does not answer the
51
+ unstabilized question. There are also substantial positive results
52
+ for particular fundamental groups. Hambleton~\cite[Theorem~B]{Hambleton18}
53
+ proves the $D(2)$ property for finite subgroups of $\operatorname{SO}(3)$.
54
+ More recently, Hofmann and Nicholson~\cite[Theorem~A]{HofmannNicholson27}
55
+ establish the $D(2)$ property for the generalized quaternion groups of
56
+ orders $24$ and $32$ and recover the order-$28$ case previously proved
57
+ using work of Mannan--Popiel and Nicholson~\cite{MannanPopiel21,Nicholson21}.
58
+ In particular,
59
+ they show that the longstanding candidate
60
+ with fundamental group of order $32$, proposed by Cohen and Dyer,
61
+ does have a finite two-dimensional model.
62
+
63
+ Candidate counterexamples have also come from relation modules.
64
+ A relation gap occurs when the relator subgroup of a free group needs
65
+ more normal generators than its abelianization needs as a module over
66
+ the quotient group ring.
67
+ Bridson and Tweedale~\cite[Sections~3--4]{BridsonTweedale07} use
68
+ coprime annihilation relations to reduce the number of module generators
69
+ and construct finite $D(2)$ complexes with virtually free fundamental
70
+ groups. Their failure to have finite two-dimensional models is conditional
71
+ on a relation-gap assertion.
72
+
73
+ We apply Quillen's plus construction~\cite{Quillen71}. It kills a
74
+ perfect normal subgroup of the fundamental
75
+ group while preserving homology with coefficients from the quotient.
76
+ Mannan~\cite[Section~2]{Mannan09} shows directly that applying it to a
77
+ finite two-dimensional complex along a finitely normally generated
78
+ perfect subgroup produces a finite $D(2)$ complex. He also proves
79
+ that every finite cohomologically two-dimensional three-dimensional
80
+ complex arises in this way up to homotopy
81
+ \cite[Theorem~3.4]{Mannan09}. Thus this construction supplies the
82
+ dimension condition; the task is to find an obstruction to a
83
+ two-dimensional model of its result.
84
+
85
+ Our obstruction uses a character. For a connected space $Y$, a
86
+ homomorphism $\rho:\pi_1(Y)\to\C^\times$ determines a
87
+ one-dimensional complex local system $L_\rho$. We prove that, when
88
+ $Y$ is a finite two-dimensional complex,
89
+ \begin{equation}\label{eq:obstruction-overview}
90
+ H_2(Y;L_\rho)=0
91
+ \quad\Longrightarrow\quad
92
+ \rho(g)=1\ \text{for every finite-order }g\in\pi_1(Y).
93
+ \end{equation}
94
+ The proof gives the stronger statement that every map $F\to Y$ from
95
+ a finite connected simplicial complex with $b_1(F;\Q)=0$ pulls $L_\rho$
96
+ back to a system with trivial monodromy. The method is a tower of
97
+ infinite cyclic covers and image subcomplexes, following the cyclic-tower
98
+ method of Howie~\cite{Howie81Pairs}; see also the formulation of
99
+ Louder--Wilton~\cite[Section~3]{LouderWilton17} and its account of
100
+ the earlier work of Papakyriakopoulos and Stallings. The additional input
101
+ is that vanishing of rank-one twisted second homology persists under
102
+ these cyclic covers, by a Laurent-polynomial rank argument.
103
+
104
+ \subsection{Proof structure}
105
+
106
+ Section~\ref{sec:tower} establishes this obstruction independently
107
+ of the construction. If a map $F\to Y$ violated it, its finite image
108
+ would have nonpositive Euler characteristic and hence admit an
109
+ infinite cyclic cover. The map lifts because $b_1(F;\Q)=0$.
110
+ Twisted second homology still vanishes upstairs, so the argument
111
+ can be repeated. Each lifted image contains strictly more simplices,
112
+ although all are images of the same fixed triangulated $F$. This
113
+ forces a contradiction.
114
+
115
+ Section~\ref{sec:plus} presents the finite plus construction with
116
+ its explicit cellular splitting. Section~\ref{sec:construction}
117
+ then gives a five-generator, four-relator presentation and a perfect
118
+ normal subgroup generated normally by two powers. The quotient has
119
+ an element of order two detected by a complex character. An exact
120
+ four-row boundary calculation shows that the presentation complex
121
+ has zero second homology with that character. The plus construction
122
+ preserves this vanishing and gives the required finite $D(2)$
123
+ complex. Equation~\eqref{eq:obstruction-overview} excludes its
124
+ two-dimensional realization.
125
+
126
+ The geometric obstruction and the finite plus construction play separate
127
+ roles: the former applies to any rank-one local system on a finite
128
+ two-dimensional complex, while the latter is standard once a suitable
129
+ perfect normal subgroup is available. Their combination makes the
130
+ failure of two-dimensional realization visible in a small twisted
131
+ cellular boundary matrix.
preprints/A-Counterexample-to-Walls-D2-Problem-October-6-2026/build/sections/02-tower.tex ADDED
@@ -0,0 +1,257 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{A tower obstruction in dimension two}
2
+ \label{sec:tower}
3
+
4
+ We first isolate the obstruction to a finite two-dimensional model.
5
+ Its input is the vanishing of second homology with a rank-one local
6
+ system. Its conclusion restricts the maps into the complex from finite
7
+ complexes with vanishing first rational Betti number. The case of a
8
+ Moore complex will then show that the corresponding character cannot
9
+ detect a finite-order element.
10
+
11
+ A \emph{rank-one complex local system} $L$ on a connected CW complex $T$
12
+ assigns a one-dimensional complex vector space to each point, with
13
+ parallel transport along paths that depends only on homotopy relative to
14
+ the endpoints. After choosing a basepoint and a basis of its fiber,
15
+ its monodromy is a character
16
+ \[
17
+ \rho:\pi_1(T)\longrightarrow\C^\times.
18
+ \]
19
+ We use ordinary homology with these coefficients. In module notation,
20
+ write $\C_\rho$ for the right $\Z[\pi_1(T)]$-module with
21
+ $v\cdot g=\rho(g)v$. If the universal-cover cellular chains carry the
22
+ left deck action, then
23
+ \[
24
+ C_*(T;L)
25
+ =\C_\rho\otimes_{\Z[\pi_1(T)]}C_*(\widetilde T;\Z).
26
+ \]
27
+ Thus cellular chains have finite support, even when $T$ is infinite.
28
+ Equivalently, $C_j(T;L)$ is the direct sum of one coefficient fiber for
29
+ each oriented $j$-cell, with boundary maps defined by parallel transport.
30
+
31
+ Two elementary consequences will be used throughout the proof. First,
32
+ if $A\subseteq T$ is a subcomplex and $\dim T\leq2$, then
33
+ \begin{equation}
34
+ H_2(A;L|_A)\longrightarrow H_2(T;L)
35
+ \quad\text{is injective}.
36
+ \label{eq:subcomplex-injection}
37
+ \end{equation}
38
+ Indeed, the cellular chain inclusion is injective, and in dimension at
39
+ most two the second homology is the kernel of the second boundary.
40
+ This argument requires no injectivity of $\pi_1(A)\to\pi_1(T)$.
41
+ Second, on a connected complex the zeroth homology is the space of
42
+ coinvariants,
43
+ \[
44
+ H_0(T;L)
45
+ =\C/\langle (\rho(g)-1)v:g\in\pi_1(T),\ v\in\C\rangle.
46
+ \]
47
+ Consequently, nontrivial monodromy implies $H_0(T;L)=0$.
48
+
49
+ The next lemma ensures that vanishing of second homology also survives
50
+ the covering operation needed in the tower.
51
+
52
+ \begin{lemma}[Infinite cyclic covers]
53
+ \label{lem:cyclic-cover}
54
+ Let $A$ be a finite connected CW complex of dimension at most two, let
55
+ $L$ be a rank-one complex local system on $A$, and let
56
+ $p:\widehat A\to A$ be a connected infinite cyclic cover. If
57
+ $H_2(A;L)=0$, then
58
+ \[
59
+ H_2(\widehat A;p^*L)=0.
60
+ \]
61
+ \end{lemma}
62
+
63
+ \begin{proof}
64
+ Choose a generator $\tau$ of the deck group and put
65
+ $R=\C[z,z^{-1}]$. There is a canonical deck action on the pulled-back
66
+ local system: in the fiber description of $p^*L$, it is
67
+ \begin{equation}
68
+ (\widehat x,v)\longmapsto(\tau\widehat x,v),
69
+ \qquad v\in L_{p(\widehat x)}.
70
+ \label{eq:canonical-deck-action}
71
+ \end{equation}
72
+ The equality $p\tau=p$ makes this action compatible with parallel
73
+ transport. Let $z$ act by this deck transformation. Choosing one lift
74
+ of each cell of $A$ and a basis in its coefficient fiber identifies
75
+ $C_j(\widehat A;p^*L)$ with a finite free $R$-module, of rank equal to
76
+ the number of $j$-cells of $A$.
77
+
78
+ Taking coinvariants of this deck action identifies translated cell
79
+ lifts and their coefficient fibers. It therefore gives an isomorphism
80
+ of chain complexes
81
+ \begin{equation}
82
+ C_*(\widehat A;p^*L)\otimes_R R/(z-1)
83
+ \cong C_*(A;L).
84
+ \label{eq:cyclic-specialization}
85
+ \end{equation}
86
+ In the chosen bases, let $D(z)$ be the matrix of the second boundary
87
+ upstairs, and let $m$ be its number of columns. The matrix $D(1)$ is
88
+ the second boundary downstairs, so it is injective by the hypothesis.
89
+ If $m=0$, there is nothing to prove. Otherwise, some $m\times m$ minor
90
+ of $D(1)$ is nonzero. The corresponding minor of $D(z)$ is consequently
91
+ a nonzero Laurent polynomial. Thus $D(z)$ has full column rank over
92
+ $\C(z)$ and is injective over $R$, since $R^m$ embeds in $\C(z)^m$.
93
+ There are no cells above dimension two, and hence
94
+ $H_2(\widehat A;p^*L)=\ker D(z)=0$.
95
+ \end{proof}
96
+
97
+ The following proof adapts the cyclic-tower method of
98
+ Howie~\cite{Howie81Pairs}, in which one alternates subcomplex inclusions
99
+ and infinite cyclic covers; see Louder--Wilton~\cite[Section~3]{LouderWilton17}.
100
+ Lemma~\ref{lem:cyclic-cover} supplies the property that persists along
101
+ the tower here: vanishing of twisted second homology.
102
+
103
+ \begin{theorem}[Tower obstruction]
104
+ \label{thm:tower}
105
+ Let $Y$ be a finite connected CW complex of dimension at most two, and
106
+ let $L$ be a rank-one complex local system on $Y$ with $H_2(Y;L)=0$.
107
+ There is no map $f:F\to Y$ from a finite connected simplicial complex
108
+ satisfying $b_1(F;\Q)=0$ for which $f^*L$ has nontrivial monodromy.
109
+ \end{theorem}
110
+
111
+ \begin{proof}
112
+ Suppose that such a map exists. We will repeatedly lift it to an
113
+ infinite cyclic cover and replace that cover by the image of the lift.
114
+ At every step the image will contain strictly more simplices, although
115
+ the domain retains one fixed finite triangulation. For a finite
116
+ simplicial complex $A$, write $s(A)$ for its number of nonempty simplices.
117
+
118
+ We first justify working simplicially without increasing the dimension
119
+ of $Y$. Its one-skeleton is a finite graph. Subdivide that graph to
120
+ make it simplicial and homotope each two-cell attaching map to an edge
121
+ path. After further subdivision if necessary, each nonconstant
122
+ attaching path can be represented by a map from a polygonal circle
123
+ with at least three edges, with every edge mapping homeomorphically
124
+ onto a graph edge. Replace the attachment by the mapping cylinder of this
125
+ map, capped by a disk along its free boundary circle. This merely
126
+ inserts a collar into the attached disk. The resulting cylinder has
127
+ one rectangle for each traversal of a graph edge. Each rectangle is
128
+ embedded, with its two upper vertices in the separate domain circle
129
+ and its two lower vertices at distinct endpoints of the graph edge.
130
+ After compatible subdivisions of boundary edges, triangulate each
131
+ rectangle from its own interior vertex and each capping disk from a
132
+ new interior vertex. This yields a finite simplicial complex even
133
+ when different rectangles traverse the same graph edge: their
134
+ interiors and upper edges remain distinct. A constant attaching map
135
+ contributes a triangulated two-sphere joined to the graph at one
136
+ vertex. Homotoping the attaching maps preserves the homotopy type,
137
+ so this construction gives a finite simplicial model of dimension at
138
+ most two.
139
+
140
+ Transfer $L$ and $f$ across this homotopy equivalence. Homotopy
141
+ invariance preserves both $H_2(Y;L)=0$ and the nontrivial pullback
142
+ monodromy. After a sufficiently fine subdivision of $F$, simplicial
143
+ approximation makes $f$ simplicial. Fix this triangulation of $F$
144
+ for the rest of the proof. Let $A_0=f(F)$, let $f_0:F\to A_0$ be the
145
+ corestriction, and let $L_0=L|_{A_0}$. The simplicial image $A_0$ is
146
+ a finite connected subcomplex, and
147
+ \eqref{eq:subcomplex-injection} gives $H_2(A_0;L_0)=0$.
148
+
149
+ Here is the inductive step. Suppose that $A_i$ is a finite connected
150
+ simplicial complex of dimension at most two, $f_i:F\to A_i$ is a
151
+ simplicial map onto its image $A_i$, and $L_i$ satisfies
152
+ \begin{equation}
153
+ H_2(A_i;L_i)=0,
154
+ \qquad f_i^*L_i\text{ has nontrivial monodromy}.
155
+ \label{eq:tower-invariants}
156
+ \end{equation}
157
+ The second condition implies that $L_i$ itself has nontrivial
158
+ monodromy, so $H_0(A_i;L_i)=0$. Since rank-one cellular chains have
159
+ the same dimensions as ordinary complex cellular chains, the Euler
160
+ characteristic gives
161
+ \[
162
+ \chi(A_i)=-\dim_\C H_1(A_i;L_i)\leq0.
163
+ \]
164
+ On the other hand,
165
+ \[
166
+ \chi(A_i)=1-b_1(A_i;\Q)+b_2(A_i;\Q).
167
+ \]
168
+ It follows that $b_1(A_i;\Q)\geq1$. The finitely generated
169
+ abelianization of $\pi_1(A_i)$ therefore has a nonzero free part,
170
+ and there is an epimorphism
171
+ $\phi_i:\pi_1(A_i)\twoheadrightarrow\Z$.
172
+
173
+ Let $p_i:\widehat A_i\to A_i$ be the connected cover corresponding to
174
+ $\ker\phi_i$. The composite $\phi_i(f_i)_*$ is zero: every
175
+ homomorphism $\pi_1(F)\to\Z$ factors through $H_1(F;\Z)$, which is
176
+ finite because $F$ is finite and $b_1(F;\Q)=0$.
177
+ Thus $f_i$ lifts to $\widetilde f_i:F\to\widehat A_i$.
178
+ Give the cover the lifted triangulation. The lift is simplicial on
179
+ the already fixed triangulation of $F$, since on each domain simplex
180
+ it is the lift of a simplicial map into a single target simplex.
181
+ No new subdivision of $F$ is needed.
182
+
183
+ Set
184
+ \[
185
+ A_{i+1}=\widetilde f_i(F),
186
+ \qquad L_{i+1}=(p_i^*L_i)|_{A_{i+1}},
187
+ \]
188
+ and corestrict the lift to $f_{i+1}:F\to A_{i+1}$.
189
+ Lemma~\ref{lem:cyclic-cover}, followed by
190
+ \eqref{eq:subcomplex-injection}, gives
191
+ $H_2(A_{i+1};L_{i+1})=0$. Moreover,
192
+ $f_{i+1}^*L_{i+1}\cong f_i^*L_i$, so the nontrivial monodromy
193
+ persists. These are precisely the conditions
194
+ \eqref{eq:tower-invariants} needed to continue. Figure~\ref{fig:tower}
195
+ shows one step.
196
+
197
+ \begin{figure}[tb]
198
+ \centering
199
+ \input{figures/tower}
200
+ \caption{One step of the tower. The lifted map factors through its
201
+ finite image $A_{i+1}\subseteq\widehat A_i$, and the diagram commutes.
202
+ The domain $F$ keeps the same triangulation at every step; only the
203
+ indicated subcomplex arrow is an inclusion.}
204
+ \label{fig:tower}
205
+ \end{figure}
206
+
207
+ It remains to show that $s(A_i)$ increases strictly. The restriction
208
+ $p_i|_{A_{i+1}}$ maps onto $A_i$ and maps each
209
+ simplex isomorphically onto a simplex. Hence
210
+ $s(A_{i+1})\geq s(A_i)$. If equality held, there would be exactly
211
+ one simplex above each simplex of $A_i$, compatibly with all faces.
212
+ The restriction would then be a simplicial isomorphism. Its inverse,
213
+ followed by the inclusion into $\widehat A_i$, would give a section
214
+ of $p_i$. Such a section would make $(p_i)_*$ surjective, contrary
215
+ to
216
+ \[
217
+ \im(p_i)_*=\ker\phi_i\ne\pi_1(A_i).
218
+ \]
219
+ Thus $s(A_{i+1})>s(A_i)$. But every simplex of $A_i$ is the image
220
+ of a simplex in the fixed triangulation of $F$, so
221
+ \[
222
+ s(A_0)<s(A_1)<s(A_2)<\cdots\leq s(F).
223
+ \]
224
+ This is impossible, and the theorem follows.
225
+ \end{proof}
226
+
227
+ \Needspace{5\baselineskip}
228
+ The following consequence is the form used in the construction.
229
+
230
+ \begin{corollary}[Characters and torsion]
231
+ \label{cor:torsion}
232
+ Let $Y$ be a finite connected CW complex of dimension at most two.
233
+ If a character $\rho:\pi_1(Y)\to\C^\times$ satisfies
234
+ $H_2(Y;\C_\rho)=0$, then $\rho(g)=1$ for every finite-order
235
+ element $g\in\pi_1(Y)$.
236
+ \end{corollary}
237
+
238
+ \begin{proof}
239
+ Suppose that $g$ has finite order $n$ and $\rho(g)\ne1$; in
240
+ particular, $n\geq2$. Let
241
+ \[
242
+ M_n=S^1\cup_{\deg n}D^2
243
+ \]
244
+ be the Moore complex obtained by attaching a disk along a map of
245
+ degree $n$. A loop in $Y$ representing $g$ extends to a map
246
+ $M_n\to Y$, because its $n$th power is nullhomotopic. The cellular
247
+ boundary $C_2(M_n;\Z)\to C_1(M_n;\Z)$ is multiplication by $n$,
248
+ so $H_1(M_n;\Z)=\Z/n$ and $b_1(M_n;\Q)=0$. The pullback
249
+ character sends the circle generator to $\rho(g)\ne1$.
250
+
251
+ Use the finite simplicial model for $M_n$ constructed in the proof of
252
+ Theorem~\ref{thm:tower}, and compose its homotopy equivalence to
253
+ $M_n$ with the map to $Y$. This gives a finite connected simplicial
254
+ domain with vanishing first rational Betti number and nontrivial
255
+ pullback monodromy, contradicting that theorem. For $n=2$ the
256
+ standard model $M_2$ is $\RP^2$, the case needed below.
257
+ \end{proof}
preprints/A-Counterexample-to-Walls-D2-Problem-October-6-2026/build/sections/03-plus.tex ADDED
@@ -0,0 +1,117 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{A finite plus construction}\label{sec:plus}
2
+
3
+ We next recall how a finitely normally generated perfect subgroup
4
+ produces a finite $D(2)$ complex. This is the finite form of Quillen's
5
+ plus construction~\cite{Quillen71} used by Mannan~\cite[Section~2]{Mannan09}.
6
+ We give the construction because its cellular splitting proves both
7
+ the required cohomological vanishing and the preservation of the twisted
8
+ homology used in Section~\ref{sec:tower}.
9
+
10
+ Recall that a group $K$ is \emph{perfect} if $K=[K,K]$, or equivalently
11
+ if its abelianization $K_{\ab}$ is zero. A normal subgroup of a group
12
+ $P$ is \emph{finitely normally generated} if it is the normal closure
13
+ in $P$ of finitely many elements. This condition does not require
14
+ finite generation as an abstract group.
15
+
16
+ \begin{proposition}[Finite plus construction]\label{prop:plus}
17
+ Let $B$ be a finite connected CW complex of dimension at most two,
18
+ with $\pi_1(B)=P$. Suppose that the normal closure $K$ of elements
19
+ $t_1,\ldots,t_r\in P$ is perfect, and put $G=P/K$.
20
+ There is a finite complex $X\supseteq B$, obtained by attaching
21
+ $r$ cells of dimension two and $r$ cells of dimension three, such that:
22
+ \begin{enumerate}
23
+ \item the inclusion induces the quotient $P\to G$ on fundamental groups;
24
+ \item $H_i(\widetilde X;\Z)=0$ for every $i>2$, and
25
+ $H^3(X;M)=0$ for every left $\Z G$-module $M$;
26
+ \item for every right $\Z G$-module $N$, the inclusion induces
27
+ $H_*(B;N)\cong H_*(X;N)$, with the coefficients on $B$
28
+ pulled back along $P\to G$.
29
+ \end{enumerate}
30
+ \end{proposition}
31
+
32
+ \begin{proof}
33
+ Attach two-dimensional cells along loops representing $t_1,\ldots,t_r$,
34
+ and call the resulting complex $B'$. The van Kampen theorem gives
35
+ $\pi_1(B')=G$. Let $\overline B$ be the full preimage of $B$ in the
36
+ universal cover $\widetilde{B'}$. Since $P\to G$ is onto,
37
+ $\overline B$ is connected; it is the covering of $B$ corresponding
38
+ to $K$. Hence
39
+ \[
40
+ H_1(\overline B;\Z)=K_{\ab}=0.
41
+ \]
42
+
43
+ Write $R=\Z G$ and regard cellular chains of these covers as left
44
+ $R$-modules. The relative cellular complex
45
+ $C_*(\widetilde{B'},\overline B)$ consists of $R^r$ in degree two
46
+ and zero in every other degree. The homology exact sequence of the
47
+ pair therefore gives a surjection
48
+ \begin{equation}\label{eq:relative-surjection}
49
+ H_2(\widetilde{B'};\Z)
50
+ \longrightarrow H_2(\widetilde{B'},\overline B;\Z)=R^r.
51
+ \end{equation}
52
+ Choose classes $\alpha_1,\ldots,\alpha_r$ mapping to the standard
53
+ basis vectors, where the basis records chosen lifts and orientations
54
+ of the new cells. The space $\widetilde{B'}$ is simply connected, so
55
+ the degree-two Hurewicz theorem represents each $\alpha_j$ by a map
56
+ $S^2\to\widetilde{B'}$. Project these maps to $B'$ and attach one
57
+ three-dimensional cell along each projected map. This defines $X$.
58
+ Only finitely many cells have been added, and attaching the last cells
59
+ does not change the fundamental group.
60
+
61
+ The preimage of $B'$ in $\widetilde X$ is its universal cover, so we
62
+ may retain the notation $\widetilde{B'}$ and $\overline B$. In the
63
+ chosen cellular bases,
64
+ \[
65
+ C_3(\widetilde X)=R^r,
66
+ \qquad C_2(\widetilde X)=C_2(\overline B)\oplus R^r.
67
+ \]
68
+ Let $q:C_2(\widetilde X)\to R^r$ be projection onto the second
69
+ summand. The choice in \eqref{eq:relative-surjection} says exactly that
70
+ \begin{equation}\label{eq:split-boundary}
71
+ q\,\partial_3=\id_{R^r}.
72
+ \end{equation}
73
+ Indeed, the relative cellular boundary of the $j$th three-dimensional
74
+ cell is the $j$th basis vector; in the two-dimensional complex
75
+ $\widetilde{B'}$, a homology class is represented by its cellular
76
+ two-cycle without any ambiguity from three-boundaries.
77
+
78
+ Equation~\eqref{eq:split-boundary} proves that $\partial_3$ is
79
+ injective. There are no cells above dimension three, so
80
+ $H_i(\widetilde X;\Z)=0$ for all $i>2$. It also gives the
81
+ cohomological assertion directly. For any $R$-linear map
82
+ $\varphi:C_3(\widetilde X)\to M$, its extension
83
+ $\varphi q:C_2(\widetilde X)\to M$ satisfies
84
+ \[
85
+ (\varphi q)\partial_3=\varphi.
86
+ \]
87
+ Thus the cochain boundary
88
+ $\Hom_R(C_2(\widetilde X),M)\to\Hom_R(C_3(\widetilde X),M)$
89
+ is onto, and $H^3(X;M)=0$.
90
+
91
+ Finally, the relative cellular complex of $(\widetilde X,\overline B)$
92
+ is
93
+ \begin{equation}\label{eq:relative-complex}
94
+ 0\longrightarrow R^r\xrightarrow{\,\id\,}R^r
95
+ \longrightarrow0,
96
+ \end{equation}
97
+ in degrees three and two. It is contractible. The short exact sequence
98
+ of absolute and relative cellular complexes is split in each degree,
99
+ since the cells of $\overline B$ form subsets of the chosen cellular
100
+ bases. Tensoring with any right $R$-module $N$ therefore leaves a short
101
+ exact sequence of complexes whose relative term is still contractible.
102
+ Its homology exact sequence gives
103
+ \[
104
+ H_*(N\otimes_R C_*(\overline B))
105
+ \cong H_*(N\otimes_R C_*(\widetilde X)).
106
+ \]
107
+ The left side computes $H_*(B;N)$: the coefficient action of $P$
108
+ factors through the deck group $G$ of $\overline B\to B$.
109
+ The right side computes $H_*(X;N)$, proving the last assertion.
110
+ \end{proof}
111
+
112
+ The splitting in \eqref{eq:split-boundary} is stronger than ordinary
113
+ third-homology vanishing: it makes the cohomology calculation work for
114
+ every coefficient module. In the application, we will choose $B$ and
115
+ $K$ so that a character of $G$ has vanishing second homology on $B$,
116
+ yet detects a torsion element of $G$. Proposition~\ref{prop:plus}
117
+ preserves that homology vanishing when passing to $X$.
preprints/A-Counterexample-to-Walls-D2-Problem-October-6-2026/build/sections/04-construction.tex ADDED
@@ -0,0 +1,189 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{The counterexample}\label{sec:construction}
2
+
3
+ We now construct the presentation complex and perfect normal subgroup
4
+ needed in Proposition~\ref{prop:plus}. The quotient must contain torsion
5
+ detected by a character, and the corresponding local system on the
6
+ presentation complex must have vanishing second homology.
7
+ Perfectness will follow from
8
+ annihilation relations with coprime coefficients in the subgroup's
9
+ abelianization.
10
+ Related uses of coprime annihilators for relation modules appear in
11
+ Bridson--Tweedale~\cite[Proposition~3.3]{BridsonTweedale07}.
12
+
13
+ Let $B$ be the presentation complex of
14
+ \begin{equation}\label{eq:presentation}
15
+ P=\left\langle x_1,a_1,x_2,a_2,s\ \middle|\
16
+ \begin{aligned}
17
+ x_1a_1x_1^{-1}&=a_1^4,&
18
+ x_2a_2x_2^{-1}&=a_2^3,\\
19
+ x_1&=a_2^{13},&
20
+ s x_2 s^{-1}&=a_1^5
21
+ \end{aligned}\right\rangle.
22
+ \end{equation}
23
+ Thus $B$ has one vertex, five edges, and four two-dimensional cells.
24
+ Define
25
+ \[
26
+ t_1=x_1^2,\qquad t_2=x_2^3,\qquad
27
+ K=\langle\!\langle t_1,t_2\rangle\!\rangle_P,
28
+ \qquad G=P/K,
29
+ \]
30
+ where the double brackets denote normal closure in $P$.
31
+ Sending $s$ to $1\in\Z$ and the other four generators to zero
32
+ respects all these relations and descends to an epimorphism
33
+ $G\to\Z$. In particular, $G$ is infinite.
34
+ We use the commutator convention $[g,h]=ghg^{-1}h^{-1}$.
35
+
36
+ \begin{lemma}\label{lem:perfect}
37
+ The normal subgroup $K$ is perfect.
38
+ \end{lemma}
39
+
40
+ \begin{proof}
41
+ The exponents are matched by $4^2-1=15=3\cdot5$ and
42
+ $3^3-1=26=2\cdot13$, with $\gcd(15,26)=1$.
43
+ Conjugation by $t_1=x_1^2$ sends $a_1$ to $a_1^{16}$, while
44
+ conjugation by $t_2=x_2^3$ sends $a_2$ to $a_2^{27}$.
45
+ Squaring $x_1=a_2^{13}$ and cubing $s x_2s^{-1}=a_1^5$ now give
46
+ \begin{equation}\label{eq:commutators}
47
+ t_1=a_2^{26}=[t_2,a_2],
48
+ \qquad
49
+ s t_2 s^{-1}=a_1^{15}=[t_1,a_1].
50
+ \end{equation}
51
+ Write $K_{\ab}$ additively and let $u_j$ be the image of $t_j$.
52
+ Conjugation makes $K_{\ab}$ a left $\Z G$-module: every element
53
+ of $K$ acts trivially on its own abelianization. For $t\in K$,
54
+ the image of $[t,a]$ is $(1-a)[t]$. Consequently
55
+ \begin{equation}\label{eq:module-relations}
56
+ u_1=(1-a_2)u_2,
57
+ \qquad s u_2=(1-a_1)u_1.
58
+ \end{equation}
59
+
60
+ Since $t_1=a_2^{26}$, the element $a_2$ fixes $u_1$ and
61
+ $a_2^{26}$ acts trivially on all of $K_{\ab}$. Applying
62
+ $1+a_2+\cdots+a_2^{25}$ to the first equality gives
63
+ \[
64
+ 26u_1=(1-a_2^{26})u_2=0.
65
+ \]
66
+ Likewise, $a_1$ fixes $s u_2$, because $s t_2s^{-1}=a_1^{15}$;
67
+ and $a_1^{15}$ acts trivially on $K_{\ab}$. Applying
68
+ $1+a_1+\cdots+a_1^{14}$ to the second equality gives
69
+ \[
70
+ 15s u_2=(1-a_1^{15})u_1=0.
71
+ \]
72
+ The action of $s$ is invertible, so $15u_2=0$, and the first
73
+ equality of \eqref{eq:module-relations} then gives $15u_1=0$.
74
+ Since $15$ and $26$ are relatively prime, $u_1=0$. The second
75
+ equality gives $s u_2=0$, hence $u_2=0$.
76
+
77
+ Every element of $K$ is a product of $P$-conjugates of $t_1^{\pm1}$
78
+ and $t_2^{\pm1}$. Thus $u_1,u_2$ generate $K_{\ab}$ under
79
+ addition and the $P$-action. Their vanishing proves $K_{\ab}=0$.
80
+ \end{proof}
81
+
82
+ By Proposition~\ref{prop:plus}, there is a finite complex $X\supseteq B$
83
+ with fundamental group $G$, obtained by adding two two-dimensional
84
+ and two three-dimensional cells, such that
85
+ \begin{equation}\label{eq:d2-for-x}
86
+ H_i(\widetilde X;\Z)=0\quad(i>2),\qquad
87
+ H^3(X;M)=0\quad\text{for every left }\Z G\text{-module }M.
88
+ \end{equation}
89
+ It remains to find the character that obstructs a two-dimensional model.
90
+
91
+ Choose a primitive third root of unity $\zeta\in\C$. The assignments
92
+ \begin{equation}\label{eq:character}
93
+ \rho(x_1)=-1,\quad \rho(a_1)=\zeta,\quad
94
+ \rho(x_2)=\zeta^2,\quad \rho(a_2)=-1,\quad \rho(s)=1
95
+ \end{equation}
96
+ satisfy the four relations of \eqref{eq:presentation}, since
97
+ \[
98
+ \zeta=\zeta^4,\qquad -1=(-1)^3,\qquad
99
+ -1=(-1)^{13},\qquad \zeta^2=\zeta^5.
100
+ \]
101
+ They also send $t_1$ and $t_2$ to $1$. Hence they define a character
102
+ $\rho:G\to\C^\times$. Denote its local system on $X$ and its
103
+ pullback to $B$ by $L_\rho$.
104
+
105
+ \Needspace{6\baselineskip}
106
+ \begin{lemma}\label{lem:twisted-vanishing}
107
+ The local system $L_\rho$ satisfies $H_2(X;L_\rho)=0$.
108
+ \end{lemma}
109
+
110
+ \begin{proof}
111
+ Proposition~\ref{prop:plus} reduces the computation to $B$.
112
+ Its twisted cellular groups in degrees two and one are $\C^4$ and
113
+ $\C^5$, respectively. We compute the second boundary by the lifted
114
+ edge-path sum, equivalently by Fox differentiation~\cite{Fox53}.
115
+ In this convention the derivative of a word obeys
116
+ \[
117
+ \frac{\partial(uv)}{\partial g}
118
+ =\frac{\partial u}{\partial g}
119
+ +u\frac{\partial v}{\partial g},\qquad
120
+ \frac{\partial g}{\partial g}=1,\qquad
121
+ \frac{\partial g^{-1}}{\partial g}=-g^{-1},
122
+ \]
123
+ and the derivatives with respect to other generators are zero.
124
+ Evaluate their group-ring coefficients at $\rho$.
125
+
126
+ Use the relators
127
+ \[
128
+ \begin{split}
129
+ r_1&=x_1a_1x_1^{-1}a_1^{-4},\qquad
130
+ r_2=x_2a_2x_2^{-1}a_2^{-3},\\
131
+ r_3&=x_1a_2^{-13},\qquad
132
+ r_4=sx_2s^{-1}a_1^{-5}.
133
+ \end{split}
134
+ \]
135
+ With the edges ordered as $x_1,a_1,x_2,a_2,s$, the four boundary
136
+ vectors, written as rows, are
137
+ \begin{equation}\label{eq:fox-matrix}
138
+ D=\begin{pmatrix}
139
+ 1-\zeta & -2 & 0 & 0 & 0\\
140
+ 0&0&2&\zeta^2-1&0\\
141
+ 1&0&0&-1&0\\
142
+ 0&-(1+\zeta)&1&0&1-\zeta^2
143
+ \end{pmatrix}.
144
+ \end{equation}
145
+ Here is a direct check of the entries. For a relator
146
+ $xax^{-1}a^{-n}$, the evaluated entries in the $x$ and $a$
147
+ coordinates are
148
+ \[
149
+ 1-\rho(a)^n,
150
+ \qquad \rho(x)-\sum_{j=0}^{n-1}\rho(a)^j.
151
+ \]
152
+ For $r_1$, the latter sum is
153
+ $1+\zeta+\zeta^2+\zeta^3=1$; for $r_2$, it is $1-1+1=1$.
154
+ For $r_3$, the alternating sum of thirteen terms is $1$.
155
+ For $r_4$, the $a_1$ entry is
156
+ $-\sum_{j=0}^4\zeta^j=-(1+\zeta)$, the $x_2$ entry is
157
+ $\rho(s)=1$, and the $s$ entry is $1-\rho(x_2)=1-\zeta^2$.
158
+ These give \eqref{eq:fox-matrix}.
159
+
160
+ The minor using columns $x_1,a_1,x_2,s$ has determinant
161
+ \begin{equation}\label{eq:nonzero-minor}
162
+ -4(1-\zeta^2)\ne0.
163
+ \end{equation}
164
+ Thus the four rows are independent, so the boundary
165
+ $C_2(B;L_\rho)\to C_1(B;L_\rho)$ is injective.
166
+ Since $B$ has no three-dimensional cells, $H_2(B;L_\rho)=0$,
167
+ as required.
168
+ \end{proof}
169
+
170
+ \begin{proof}[Proof of Theorem~\ref{thm:main}]
171
+ The complex $X$ constructed above is finite and satisfies
172
+ \eqref{eq:d2-for-x}. In $G$, the element $x_1$ has square one,
173
+ and it is nonidentity because $\rho(x_1)=-1$. Thus its order is
174
+ exactly two.
175
+
176
+ Suppose that $X$ were homotopy equivalent to a finite connected
177
+ complex $Y$ of dimension at most two. Transfer $\rho$ along the
178
+ induced isomorphism of fundamental groups, giving a local system
179
+ $L$ on $Y$. Homotopy invariance and Lemma~\ref{lem:twisted-vanishing}
180
+ give $H_2(Y;L)=0$. But the transferred character takes the value
181
+ $-1$ on an element of order two, contrary to
182
+ Corollary~\ref{cor:torsion}.
183
+
184
+ Concretely, a loop representing that element extends to a map
185
+ $\RP^2\to Y$: the attaching loop of the two-dimensional cell of
186
+ $\RP^2$ is its generator traversed twice. The pulled-back local
187
+ system has monodromy $-1$, whereas $b_1(\RP^2;\Q)=0$.
188
+ This is precisely the map excluded by Theorem~\ref{thm:tower}.
189
+ \end{proof}
preprints/A-Counterexample-to-Walls-D2-Problem-October-6-2026/wall-d2-counterexample.pdf ADDED
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preprints/A-Counterexample-to-the-Group-Ring-Determinant-Conjecture-September-23-2026/README.md ADDED
@@ -0,0 +1,18 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ # [A Counterexample to the Group-Ring Determinant Conjecture](paper.pdf)
2
+
3
+ **Author:** OpenAI
4
+
5
+ **Date:** September 23, 2026
6
+
7
+ ## Citation
8
+
9
+ ```bibtex
10
+ @misc{OAI:A-Counterexample-to-the-Group-Ring-Determinant-Conjecture-September-23-2026,
11
+ author = {{OpenAI}},
12
+ title = {{A Counterexample to the Group-Ring Determinant Conjecture}},
13
+ howpublished = {OpenAI Math Release preprint
14
+ \href{https://github.com/openai/math/blob/main/preprints/A-Counterexample-to-the-Group-Ring-Determinant-Conjecture-September-23-2026/paper.pdf}{OAI:A-Counterexample-to-the-Group-Ring-Determinant-Conjecture-September-23-2026}},
15
+ year = {2026}
16
+ }
17
+ ```
18
+
preprints/A-Counterexample-to-the-Group-Ring-Determinant-Conjecture-September-23-2026/build/main.tex ADDED
@@ -0,0 +1,615 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
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+ \documentclass[11pt]{article}
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+ \usepackage[T1]{fontenc}
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+ \usepackage{lmodern}
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+ \usepackage[margin=1in]{geometry}
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+ \usepackage{amsmath,amssymb,amsthm,mathtools}
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+ \usepackage{microtype}
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+ \usepackage{xcolor}
8
+ \PassOptionsToPackage{hyphens}{url}
9
+ \usepackage{hyperref}
10
+ \usepackage{bookmark}
11
+ \hypersetup{colorlinks=true,linkcolor=blue!45!black,citecolor=blue!45!black,
12
+ urlcolor=blue!45!black,pdfauthor={OpenAI},
13
+ pdftitle={A Counterexample to the Group-Ring Determinant Conjecture}}
14
+ \input{glyphtounicode-cmex.tex}
15
+ \pdfgentounicode=1
16
+ \newtheorem{theorem}{Theorem}[section]
17
+ \newtheorem{proposition}[theorem]{Proposition}
18
+ \newtheorem{lemma}[theorem]{Lemma}
19
+ \theoremstyle{remark}
20
+ \newtheorem{remark}[theorem]{Remark}
21
+ \numberwithin{equation}{section}
22
+ \newcommand{\F}{\mathbb F}
23
+ \newcommand{\Z}{\mathbb Z}
24
+ \newcommand{\Q}{\mathbb Q}
25
+ \newcommand{\R}{\mathbb R}
26
+ \newcommand{\C}{\mathbb C}
27
+ \newcommand{\Mat}{\operatorname{M}}
28
+ \newcommand{\diag}{\operatorname{diag}}
29
+ \newcommand{\N}{\mathcal N}
30
+ \setlength{\emergencystretch}{2em}
31
+ \title{A Counterexample to the Group-Ring Determinant Conjecture}
32
+ \author{OpenAI}
33
+ \date{September 23, 2026}
34
+
35
+ \begin{document}
36
+ \maketitle
37
+ \begin{abstract}
38
+ We disprove the unrestricted group-ring Determinant Conjecture. We construct a finitely generated group $G$ and a square matrix over $\mathbb Z[G]$ that is invertible over $\mathbb Q[G]$ and has Fuglede--Kadison determinant strictly between zero and one. The logarithmic integral defining the determinant is finite.
39
+ \end{abstract}
40
+
41
+ \section{Introduction and proof overview}
42
+ \label{sec:introduction}
43
+
44
+ A nonsingular integer matrix has determinant of absolute
45
+ value at least one. The group-ring Determinant Conjecture asks for an
46
+ analogue when the entries are finite integer combinations of elements
47
+ of a discrete group. The relevant determinant, introduced by Fuglede
48
+ and Kadison~\cite{FK1952}, uses the trace of a logarithm rather than
49
+ a finite-dimensional determinant polynomial.
50
+
51
+ Here are the conventions that fix this question. Let $G$ be a discrete
52
+ group and let $\Z[G]$ denote its ordinary group ring of finite sums.
53
+ Use the left regular representation
54
+ \[
55
+ (L_g\xi)(h)=\xi(g^{-1}h),\qquad \xi\in\ell^2(G).
56
+ \]
57
+ For $A\in\Mat_n(\Z[G])$, write $T_A$ for its operator on
58
+ $\ell^2(G)^n$ and $e_i$ for the vector with $\delta_1$ in component
59
+ $i$. The probability spectral measure of the positive square is
60
+ \[
61
+ \mu_A(E)=\frac1n\sum_{i=1}^n
62
+ \langle \mathbf1_E(T_A^*T_A)e_i,e_i\rangle
63
+ \quad(E\subseteq[0,\infty)\text{ Borel}).
64
+ \]
65
+ The square-matrix instance of the conjecture is
66
+ \begin{equation}\label{eq:conjecture}
67
+ \int_{(0,\infty)}\log t\,d\mu_A(t)\ge0.
68
+ \end{equation}
69
+ The zero atom is omitted and the general integral may be $-\infty$.
70
+ The usual conjecture also permits rectangular matrices
71
+ \cite[Conjecture 13.2]{Luck2002}; a square counterexample already
72
+ contradicts it. Our example will have a bounded inverse, so its
73
+ spectrum stays away from zero.
74
+
75
+ Write $\N(G)$ for the group von Neumann algebra and use the
76
+ \emph{unnormalized} matrix trace
77
+ $\tau_n(T)=\sum_i\langle Te_i,e_i\rangle$, so $\tau_n(I_n)=n$.
78
+ For invertible $T_A$ the determinant convention is
79
+ \begin{equation}\label{eq:normalization}
80
+ \log\det_{\N(G)}(T_A)
81
+ =\frac12\tau_n\bigl(\log(T_A^*T_A)\bigr)
82
+ =\frac n2\int_{(0,\infty)}\log t\,d\mu_A(t).
83
+ \end{equation}
84
+ This extends the absolute value of the ordinary determinant.
85
+ The inversion unitary $\delta_g\mapsto\delta_{g^{-1}}$ identifies
86
+ our integral-matrix convention with right multiplication by $A^*$
87
+ on row vectors. It fixes the identity vectors, and therefore
88
+ preserves the corresponding positive-square spectral measures.
89
+
90
+ \begin{theorem}\label{thm:main}
91
+ There are a finitely generated discrete group $G_D$, an integer
92
+ $n\ge1$, and $A\in\Mat_n(\Z[G_D])$ invertible over $\Q[G_D]$ such
93
+ that
94
+ \[
95
+ 0<\det_{\N(G_D)}(T_A)<1.
96
+ \]
97
+ The integral in Equation~\eqref{eq:conjecture} is finite and strictly
98
+ negative. Thus the unrestricted group-ring Determinant Conjecture
99
+ has a negative resolution.
100
+ \end{theorem}
101
+
102
+ \paragraph{The exact existence input.}
103
+ A unital ring is directly finite if $ab=1$ implies $ba=1$.
104
+ We use the following scalar failure of direct finiteness from the
105
+ complete characteristic-two companion.
106
+
107
+ \begin{theorem}[{\cite[Theorem 1.1]{CharacteristicTwo}}]
108
+ \label{thm:input}
109
+ There exist a finite field $K_2$ of characteristic two, a finitely
110
+ generated group $H_2$, and finite sums $a_2,b_2\in K_2[H_2]$ with
111
+ $a_2b_2=1$ and $b_2a_2\ne1$.
112
+ \end{theorem}
113
+
114
+ The companion's Section~6 specifies its field, group presentation
115
+ and scalar sums by a terminating finite prescription. We use the
116
+ existence theorem, not an executed numerical instance or a
117
+ group-word decision procedure. The coefficient field is finite but
118
+ is not asserted to be $\F_2$. There is no torsion-free hypothesis;
119
+ the companion construction uses torsion. All steps after this exact
120
+ input are proved below. In particular, a result only in odd
121
+ characteristic would not supply the binary premise used here.
122
+
123
+ \paragraph{Context and mathematical ancestry.}
124
+ Determinant bounds are part of the theory of $L^2$-invariants
125
+ \cite{Luck2002}. Approximation and closure arguments established
126
+ such bounds for large classes of groups, including amenable groups
127
+ \cite[Theorem 1.21, with its erratum]{Schick2001}; Elek and Szab\'o proved the
128
+ determinant bound for sofic groups
129
+ \cite[Theorem 5]{ElekSzabo2005}. Their proof uses finite graph
130
+ approximations and the integrality of products of nonzero eigenvalues
131
+ of positive integral matrices. Our construction instead starts from
132
+ failure of direct finiteness in characteristic two. The cited sofic theorem implies, as a
133
+ separate consequence, that its resulting group is not sofic.
134
+
135
+ The lower-bound question is distinct from determinant
136
+ \emph{approximation}. Kammeyer's counterexample to a finite-quotient
137
+ limiting formula has determinant $2$ over the discrete Heisenberg
138
+ group, while its principal congruence quotients of levels $3^i$, $i\ge1$,
139
+ have determinants at most $5^{1/3}$
140
+ \cite[Theorem 2 and Section 2]{Kammeyer2026}. That discrepancy does not violate
141
+ the lower bound one.
142
+
143
+ The finite-coordinate projection construction below is related to
144
+ the commuting wreath-product projections of Dicks and Schick
145
+ \cite[Section 3]{DicksSchick2002} and of Lehner, Neuhauser and
146
+ Woess~\cite[Section 2]{LehnerNeuhauserWoess2008}. Here the
147
+ projections separate one coefficient of a binary defect; we do not
148
+ import a spectral-distribution theorem from those works. The
149
+ analytic step is the classical tracial logarithmic derivative
150
+ \cite[Lemma 2]{FK1952}, also present in the path-integral determinant
151
+ viewpoint of de la Harpe and Skandalis
152
+ \cite[Lemma 1 and Proposition 2(d)]{deLaHarpeSkandalis1984}. We give its proof and its
153
+ application to block shears locally.
154
+
155
+ \paragraph{How a binary defect produces a real trace gap.}
156
+ Set $d=[K_2:\F_2]$. Representing multiplication by field elements
157
+ on the $d$-dimensional binary vector space $K_2$ gives matrices
158
+ $X,Y\in\Mat_d(\F_2[H_2])$ with $XY=I_d$ and a nonzero idempotent
159
+ $C=I_d-YX$. One entry of $C$ has a nonzero coefficient. We enlarge
160
+ the group to
161
+ \[
162
+ G_D=\left(\bigoplus_{h\in H_2}C_3\right)\rtimes H_2,
163
+ \]
164
+ where $H_2$ acts by left translation on the coordinate labels. Averaging over the
165
+ cyclic group at one coordinate and taking complementary averages
166
+ at finitely many other coordinates isolates that coefficient.
167
+ The result is a rational orthogonal projection $P$ of size $d+1$
168
+ with trace $d+\theta$, for a positive rational number $\theta$.
169
+ Its reduction modulo two nevertheless factors through $d$ columns.
170
+ Section~\ref{sec:projection} proves the coefficient separation and
171
+ this factorization in full.
172
+
173
+ \paragraph{How the gap becomes an integral determinant.}
174
+ For a general rational projection $P$ of size $m$, suppose an odd
175
+ integer $D$ clears its denominators and $\bar P=uv$ factors through
176
+ $r$ columns over $\F_2[G]$. Choose a power $q$ of two congruent to
177
+ one modulo $D$. Section~\ref{sec:lifting} lifts the factorization modulo $q$
178
+ by a finite geometric series in a corner ring. Arbitrary integral
179
+ lifts then give an integral block matrix with an explicit rational
180
+ inverse. Section~\ref{sec:analysis} removes its two block shears
181
+ without changing the trace of the logarithm of its positive square.
182
+ The remaining diagonal matrix expands the first $r$ coordinate
183
+ summands by $q$ and contracts the range of
184
+ $P$ by $q^{-1}$, giving
185
+ \[
186
+ \log\det(T_A)=(r-\tau_m(P))\log q.
187
+ \]
188
+ Finally Section~\ref{sec:assembly} uses $r=d$ and
189
+ $\tau_{d+1}(P)=d+\theta$ to obtain the exact value $q^{-\theta}$.
190
+ The projection construction, modular lifting and trace calculation
191
+ have distinct roles; none replaces the scalar existence input.
192
+
193
+ \section{From the scalar defect to a projection}
194
+ \label{sec:projection}
195
+
196
+ We first produce the trace gap. All group-ring sums in this section
197
+ are finite, and matrix multiplication keeps the indicated order.
198
+ For a group-ring sum $c$, write $[1]c$ for its identity coefficient.
199
+ The involution $*$ inverts group elements and conjugates coefficients;
200
+ on matrices it also transposes the indices. Thus an orthogonal
201
+ projection satisfies $P=P^*=P^2$ in the regular representation.
202
+
203
+ \begin{lemma}\label{lem:binary}
204
+ Let $K_2$ be a finite field of characteristic two and $H_2$ a group.
205
+ For $d=[K_2:\F_2]$, there is an injective unital ring homomorphism
206
+ \[
207
+ \rho:K_2[H_2]\longrightarrow\Mat_d(\F_2[H_2]).
208
+ \]
209
+ For $a_2,b_2\in K_2[H_2]$ with $a_2b_2=1\ne b_2a_2$, their images $X,Y$ satisfy
210
+ $XY=I_d$ and $C:=I_d-YX\ne0$, with
211
+ \begin{equation}\label{eq:defect}
212
+ C^2=C,\qquad XC=0,\qquad CY=0.
213
+ \end{equation}
214
+ \end{lemma}
215
+
216
+ \begin{proof}
217
+ Choose a binary basis of $K_2$. The matrix of multiplication by
218
+ $\lambda\in K_2$ is a unital ring representation; it is injective
219
+ because its value on $1\in K_2$ recovers $\lambda$. Apply this map
220
+ coefficientwise to a group-ring sum. The coefficient matrices
221
+ commute with the formal group symbols, so products are preserved.
222
+ Comparing the coefficient matrix at each group element proves
223
+ injectivity. Thus $XY=I_d$ and $I_d-YX\ne0$. Now
224
+ $(YX)^2=Y(XY)X=YX$, $X(I_d-YX)=X-(XY)X=0$ and
225
+ $(I_d-YX)Y=Y-Y(XY)=0$, proving all the identities.
226
+ \end{proof}
227
+
228
+ \begin{proposition}\label{prop:separation}
229
+ Let $X,Y\in\Mat_d(\F_2[H_2])$, $d\ge1$, satisfy
230
+ $XY=I_d\ne YX$. In the group
231
+ $G_D=(\bigoplus_{h\in H_2}C_3)\rtimes H_2$, where $H_2$ acts
232
+ by left translation on coordinate labels, there is an orthogonal
233
+ projection $P\in\Mat_{d+1}(\Z[1/3][G_D])$ and a finite set
234
+ $S\subseteq H_2\setminus\{1\}$ such that
235
+ \[
236
+ \tau_{d+1}(P)=d+\theta,\qquad
237
+ \theta=\frac13\left(\frac23\right)^{|S|}>0,
238
+ \qquad \bar P=uv,
239
+ \]
240
+ where $u$ has size $(d+1)\times d$ and $v$ has size $d\times(d+1)$
241
+ over $\F_2[G_D]$. The integer $D=3^{1+|S|}$ clears all coefficients
242
+ of $P$.
243
+ \end{proposition}
244
+
245
+ \begin{proof}
246
+ Put $C=I_d-YX$. Choose an entry $C_{ij}$ and a group element
247
+ $h_0$ whose coefficient in that entry is nonzero. The coefficient
248
+ is $1$ because the field is $\F_2$. Left multiplication by
249
+ $h_0^{-1}$ therefore gives
250
+ \begin{equation}\label{eq:support}
251
+ h_0^{-1}C_{ij}=1+\sum_{s\in S}s
252
+ \end{equation}
253
+ for a finite $S\subseteq H_2\setminus\{1\}$, possibly empty.
254
+
255
+ To isolate the identity term in Equation~\eqref{eq:support}, we
256
+ seek a nonzero rational projection $p$ with $psp=0$ for every
257
+ $s\in S$. The cyclic coordinates provide complementary projections
258
+ that enforce these vanishing products. Let $z_h$ generate the cyclic
259
+ coordinate labelled by $h$ and put
260
+ \[
261
+ p_h=\frac{1+z_h+z_h^2}{3},\qquad
262
+ p=p_1\prod_{s\in S}(1-p_s).
263
+ \]
264
+ The $p_h$ are self-adjoint idempotents: averaging the nine products
265
+ in $(1+z_h+z_h^2)^2$ gives three copies of each element of $C_3$.
266
+ They commute because distinct coordinates commute. Consequently
267
+ $p=p^*=p^2$, and the displayed product shows that $3^{1+|S|}p$
268
+ is integral. This is the elementary commuting-coordinate method
269
+ in the works cited above; compare
270
+ \cite[Lemmas 3.1 and 3.4]{DicksSchick2002}.
271
+
272
+ Conjugation obeys $s p_hs^{-1}=p_{sh}$. For $s\in S$, the
273
+ product $sps^{-1}$ contains $p_s$, while $p$ contains $1-p_s$.
274
+ All these coordinate factors commute, so
275
+ \begin{equation}\label{eq:separation}
276
+ psp=p(sps^{-1})s=0.
277
+ \end{equation}
278
+ This argument does not need disjointness of the two collections of
279
+ coordinate labels. Inverse pairs or finite-order elements in $S$
280
+ cause no change.
281
+
282
+ The original coordinates $\{1\}\cup S$ are distinct. The coefficient
283
+ of the identity in their product is therefore the product of the
284
+ individual identity coefficients. Hence
285
+ \begin{equation}\label{eq:theta}
286
+ \tau_1(p)=[1]p=\frac13\prod_{s\in S}\frac23=\theta>0.
287
+ \end{equation}
288
+ For empty $S$ this means $p=p_1$ and $\theta=1/3$.
289
+
290
+ The map $\Z[1/3]\to\F_2$ is defined because $3$ is odd. Reduce
291
+ the projection modulo two and combine
292
+ Equations~\eqref{eq:support} and~\eqref{eq:separation} to obtain
293
+ \[
294
+ \bar p h_0^{-1} C_{ij}\bar p=\bar p.
295
+ \]
296
+ Let $f$ be the row of length $d$ with entry $\bar p h_0^{-1}$
297
+ at position $i$ and zero elsewhere. Let $w$ be the column with
298
+ entry $\bar p$ at position $j$ and zero elsewhere. Thus
299
+ $fCw=\bar p$. Define
300
+ \[
301
+ P=\diag(I_d,p),\qquad
302
+ u=\begin{pmatrix}X\\fC\end{pmatrix},\qquad
303
+ v=\begin{pmatrix}Y&Cw\end{pmatrix}.
304
+ \]
305
+ Using Equation~\eqref{eq:defect} in this order gives
306
+ \[
307
+ uv=\begin{pmatrix}XY&XCw\\fCY&fC^2w\end{pmatrix}
308
+ =\diag(I_d,\bar p)=\bar P.
309
+ \]
310
+ The rational trace is $d+\theta$ by Equation~\eqref{eq:theta}.
311
+ It is the rational orthogonal projection, not its binary reduction,
312
+ that has this strictly positive extra trace.
313
+ \end{proof}
314
+
315
+ We have obtained a projection of real trace greater than $d$ but a
316
+ binary factorization through $d$ columns. The next step produces
317
+ a factorization through the same number of columns modulo a power of two, so
318
+ that it can be inserted into an integral matrix.
319
+
320
+ \section{Lifting the factorization and preserving integrality}
321
+ \label{sec:lifting}
322
+
323
+ We now work with any group $G$, an orthogonal rational projection
324
+ $P\in\Mat_m(\Q[G])$, and a factorization of $\bar P$ through $r$
325
+ columns over $\F_2[G]$. Assume that an odd integer $D$ clears the
326
+ denominators of $P$. Here orthogonality means $P^2=P=P^*$, where
327
+ $*$ transposes the matrix and inverts group elements.
328
+
329
+ For a power $q>1$ of two, the trace gap suggests the absolute value
330
+ of the operator we want: expand $r$ coordinate summands by $q$ and
331
+ contract the range of $P$ by $q^{-1}$. Its
332
+ logarithmic determinant should be $(r-\tau_m(P))\log q$, which is
333
+ negative when $\tau_m(P)>r$. The difficulty is to realize this
334
+ determinant by an integral matrix. We will add block shears whose
335
+ off-diagonal entries come from a factorization of $P$ modulo $q$.
336
+ The analytic justification that these shears preserve the determinant
337
+ is given in Section~\ref{sec:analysis}.
338
+
339
+ The first lemma lifts the binary factorization to every
340
+ power $q$ of two; only idempotence is needed for this step.
341
+
342
+ \begin{lemma}\label{lem:lift}
343
+ Let $G$ be a group, $m,r\ge1$, $D$ an odd positive integer, and
344
+ $P\in\Mat_m(\Q[G])$ satisfy $P^2=P$ and
345
+ $DP\in\Mat_m(\Z[G])$. Suppose $\bar P=uv$ over $\F_2[G]$, where $u$ and $v$
346
+ have respective sizes $m\times r$ and $r\times m$. For $q=2^k$,
347
+ $k\ge1$, the reduction $e=P_q$ has a factorization
348
+ $e=u_qv_q$ of the same sizes over $(\Z/q\Z)[G]$.
349
+ \end{lemma}
350
+
351
+ \begin{proof}
352
+ Since $D$ is odd, every coefficient of $P$ has a well-defined
353
+ reduction modulo $q$. Set $\mathcal R=(\Z/q\Z)[G]$ and choose
354
+ arbitrary finite lifts $u_0,v_0$ of $u,v$ over $\mathcal R$.
355
+ In the corner ring $e\Mat_m(\mathcal R)e$, whose identity is $e$,
356
+ put
357
+ \[
358
+ Z=eu_0v_0e,\qquad W=e-Z.
359
+ \]
360
+ Modulo two, $Z$ is $\bar Puv\bar P=\bar P^3=\bar P$.
361
+ Every coefficient of $W$ is therefore even. A product of $k$
362
+ such coefficients is divisible by $2^k$, giving $W^k=0$.
363
+ This is nilpotence in the even ideal of the corner ring; the
364
+ corner ring itself need not be nilpotent.
365
+
366
+ Because $Z=e-W$, the finite geometric sum
367
+ \[
368
+ Q=e+W+\cdots+W^{k-1}
369
+ \]
370
+ satisfies $QZ=ZQ=e-W^k=e$. When $k=1$, this sum is just $e$.
371
+ Thus $Q$ is a corner inverse of $Z$, not a claimed inverse in
372
+ the entire matrix ring. Set
373
+ \[
374
+ u_q=Qeu_0,\qquad v_q=v_0e.
375
+ \]
376
+ Then $u_qv_q=Qeu_0v_0e=QZ=e$. Only finite sums and products
377
+ were used, so the resulting supports remain finite.
378
+ \end{proof}
379
+
380
+ For the integral construction, choose $q=2^k>1$ with
381
+ $q\equiv1\pmod D$. Such a power exists because two is a unit
382
+ modulo the odd integer $D$; for $D=1$, any $2^k>1$ works.
383
+ Choose integral lifts $U,V$ of the factors from Lemma~\ref{lem:lift}.
384
+ The diagonal operator with the desired expansion and contraction is
385
+ \[
386
+ J=-q^{-1}P-(I_m-P),\qquad B=\diag(qI_r,J).
387
+ \]
388
+ The minus signs leave its positive square unchanged and will produce
389
+ the subtraction $UV-P$ needed for integrality. Prescribe the
390
+ upper-left block $qI_r$ and off-diagonal blocks $V,U$. Eliminating
391
+ these off-diagonal blocks subtracts $U(qI_r)^{-1}V=UV/q$ from the
392
+ lower-right block. To leave $J$ as the Schur complement, that block
393
+ must therefore be $UV/q+J$. Thus the factorization modulo $q$ is exactly what is
394
+ needed to cancel the denominators in this block.
395
+
396
+ \begin{lemma}\label{lem:integral}
397
+ Suppose $P=P^*=P^2\in\Mat_m(\Q[G])$, an odd $D>0$ clears its
398
+ denominators, and $\bar P=uv$ factors through $r\ge1$ columns.
399
+ Let $q=2^k>1$ satisfy $q\equiv1\pmod D$. Choose arbitrary
400
+ integral lifts $U,V$ of the factors supplied by Lemma~\ref{lem:lift}.
401
+ Then
402
+ \begin{equation}\label{eq:integral-matrix}
403
+ A=\begin{pmatrix}
404
+ qI_r&V\\
405
+ U&q^{-1}\bigl(UV-P-q(I_m-P)\bigr)
406
+ \end{pmatrix}
407
+ \in\Mat_{r+m}(\Z[G])
408
+ \end{equation}
409
+ has an inverse in $\Mat_{r+m}(\Q[G])$.
410
+ \end{lemma}
411
+
412
+ \begin{proof}
413
+ The matrix $P+q(I_m-P)=qI_m+(1-q)P$ is integral because
414
+ $D\mid(q-1)$. Its reduction modulo $q$ is $e=P_q$, which is
415
+ also the reduction of $UV$. Thus every coefficient of
416
+ $UV-P-q(I_m-P)$ is an integer divisible by $q$; the bottom-right
417
+ block of Equation~\eqref{eq:integral-matrix} is integral.
418
+
419
+ For $J$ and $B$ defined above, the complementary projection identities give
420
+ $J^{-1}=-qP-(I_m-P)$. For $x\in[0,1]$ put
421
+ \[
422
+ L_x=\begin{pmatrix}I_r&0\\xU/q&I_m\end{pmatrix},\qquad
423
+ R_x=\begin{pmatrix}I_r&xV/q\\0&I_m\end{pmatrix}.
424
+ \]
425
+ Their inverses negate the off-diagonal blocks, and multiplication
426
+ without interchanging any factors gives
427
+ \begin{equation}\label{eq:path}
428
+ M(x):=L_xBR_x=
429
+ \begin{pmatrix}qI_r&xV\\xU&x^2UV/q+J\end{pmatrix}.
430
+ \end{equation}
431
+ In particular $A=M(1)$, with the rational group-ring inverse
432
+ $R_1^{-1}B^{-1}L_1^{-1}$. For general real $x$, both $M(x)$ and
433
+ its inverse lie in the real group ring and depend continuously
434
+ differentiably on $x$. No identities $PU=U$, $VP=V$, or
435
+ $V=U^*$ are required of the chosen integer lifts.
436
+ \end{proof}
437
+
438
+ The construction is integral at its endpoint, though its simplifying
439
+ path need not be integral. We
440
+ now show that this path preserves the logarithmic determinant.
441
+
442
+ \section{The trace calculation}
443
+ \label{sec:analysis}
444
+
445
+ Let $\mathcal A_n$ be the operator-norm closure of
446
+ $\Mat_n(\C[G])$ in its left regular representation. For finite
447
+ group-ring matrices define
448
+ \[
449
+ \tau_n(C)=\sum_{i=1}^n[1]C_{ii}.
450
+ \]
451
+ The identity-coefficient formula gives
452
+ $\tau_n(CD)=\tau_n(DC)$ by summing
453
+ $(C_{ij})_g(D_{ji})_{g^{-1}}$ over $i,j,g$. Moreover
454
+ $|\tau_n(C)|\le n\|C\|$ and
455
+ $\tau_n(C^*)=\overline{\tau_n(C)}$. Thus it extends to a
456
+ continuous trace on the unital $C^*$-algebra $\mathcal A_n$.
457
+
458
+ \begin{lemma}\label{lem:logderivative}
459
+ For a continuously differentiable path
460
+ $M:[0,1]\to\mathcal A_n$ of invertible elements,
461
+ \[
462
+ \frac{d}{dx}\tau_n\bigl(\log(M(x)^*M(x))\bigr)
463
+ =2\operatorname{Re}\tau_n\bigl(M'(x)M(x)^{-1}\bigr).
464
+ \]
465
+ \end{lemma}
466
+
467
+ \begin{proof}
468
+ Put $N=M^*M$. Continuity of $M$ and its inverse on the compact
469
+ interval gives constants $0<\delta<c$ with
470
+ $\delta I\le N(x)\le cI$ for all $x$. Write
471
+ $W=I-N/c$, so $\|W\|\le\rho=1-\delta/c<1$. Functional calculus
472
+ gives the uniformly norm-convergent series
473
+ \[
474
+ \log N=(\log c)I-\sum_{j\ge1}\frac{W^j}{j}.
475
+ \]
476
+ Its derivative series is also uniformly norm-convergent, since
477
+ \[
478
+ \left\|\frac{d}{dx}\frac{W^j}{j}\right\|
479
+ \le\sup_{y\in[0,1]}\|W'(y)\|\rho^{j-1}.
480
+ \]
481
+ In the derivative of $W^j$, cyclicity makes the traces of its
482
+ $j$ terms equal; commutation of $N$ and $N'$ is not assumed.
483
+ Using $W'=-N'/c$ therefore gives
484
+ \[
485
+ \frac{d}{dx}\tau_n(\log N)
486
+ =\frac1c\sum_{j\ge1}\tau_n(W^{j-1}N')
487
+ =\tau_n(N^{-1}N').
488
+ \]
489
+ Since $N'=M'^*M+M^*M'$, the second summand contributes
490
+ $\tau_n(M'M^{-1})$. Cyclicity and
491
+ $MN^{-1}=(M^*)^{-1}$ turn the first into
492
+ \[
493
+ \tau_n((M^*)^{-1}M'^*)
494
+ =\overline{\tau_n(M'M^{-1})}.
495
+ \]
496
+ Their sum is the asserted real part. This is the tracial
497
+ logarithmic derivative of~\cite[Lemma 2]{FK1952}, written with
498
+ the unnormalized trace used here.
499
+ \end{proof}
500
+
501
+ \begin{lemma}\label{lem:shears}
502
+ Let $r,m\ge1$ and let $B\in\mathcal A_{r+m}$ be invertible.
503
+ Let $S,T$ have respective sizes $m\times r$ and $r\times m$ over
504
+ the operator-norm closure of $\C[G]$. For $x\in[0,1]$, let
505
+ $L_x,R_x$ be lower and upper block shears with diagonal blocks
506
+ $I_r,I_m$ and off-diagonal blocks $xS,xT$, respectively.
507
+ Then $\tau_{r+m}(\log((L_xBR_x)^*(L_xBR_x)))$ is constant.
508
+ \end{lemma}
509
+
510
+ \begin{proof}
511
+ Write $M=L_xBR_x$. Both shears have inverses obtained by negating
512
+ their off-diagonal blocks. The ordered product rule gives
513
+ \[
514
+ M'M^{-1}=L_x'L_x^{-1}
515
+ +(L_xB)(R_x'R_x^{-1})(L_xB)^{-1}.
516
+ \]
517
+ The matrices $L_x'L_x^{-1}$ and $R_x'R_x^{-1}$ have zero diagonal
518
+ blocks, so each has trace zero. Cyclicity gives trace zero also for
519
+ the conjugate $(L_xB)(R_x'R_x^{-1})(L_xB)^{-1}$.
520
+ Lemma~\ref{lem:logderivative} now gives zero derivative.
521
+ \end{proof}
522
+
523
+ \begin{proposition}\label{prop:criterion}
524
+ Let $G$ be a discrete group, $m,r\ge1$, and let
525
+ $P=P^*=P^2\in\Mat_m(\Q[G])$. Suppose an odd $D>0$ clears its
526
+ denominators and $\bar P=uv$ with
527
+ $u\in\Mat_{m,r}(\F_2[G])$ and
528
+ $v\in\Mat_{r,m}(\F_2[G])$. For every $q=2^k>1$ congruent to one
529
+ modulo $D$, the matrix $A$ of Lemma~\ref{lem:integral} satisfies
530
+ \begin{align}
531
+ \tau_{r+m}(\log(T_A^*T_A))
532
+ &=2(r-\tau_m(P))\log q,\label{eq:criterion-trace}\\
533
+ \log\det_{\N(G)}(T_A)&=(r-\tau_m(P))\log q.
534
+ \label{eq:criterion-det}
535
+ \end{align}
536
+ It is integral and rationally invertible, and its positive-square
537
+ spectral measure has support in a compact subinterval of $(0,\infty)$.
538
+ \end{proposition}
539
+
540
+ \begin{proof}
541
+ Lemma~\ref{lem:integral} has already established integrality and
542
+ the finite-support rational inverse. Apply Lemma~\ref{lem:shears}
543
+ to Equation~\eqref{eq:path}. At $x=0$ the matrix is
544
+ $B=\diag(qI_r,-q^{-1}P-(I_m-P))$. Orthogonality gives
545
+ \[
546
+ B^*B=\diag(q^2I_r,q^{-2}P+I_m-P),\qquad
547
+ \log(B^*B)=2\log q\,\diag(I_r,-P).
548
+ \]
549
+ Taking the trace and using shear invariance proves
550
+ Equation~\eqref{eq:criterion-trace}; half this trace is
551
+ Equation~\eqref{eq:criterion-det}. The regular representation
552
+ of the rational group-ring inverse is bounded, so
553
+ \[
554
+ \|T_A^{-1}\|^{-2}I\le T_A^*T_A\le\|T_A\|^2I.
555
+ \]
556
+ Its logarithm is therefore bounded. In the probability measure
557
+ convention from the introduction this also gives
558
+ \begin{equation}\label{eq:criterion-integral}
559
+ \int_{(0,\infty)}\log t\,d\mu_A(t)
560
+ =\frac{2(r-\tau_m(P))\log q}{r+m}.
561
+ \end{equation}
562
+ \end{proof}
563
+
564
+ \section{Assembly and exact determinant}
565
+ \label{sec:assembly}
566
+
567
+ \begin{proof}[Proof of Theorem~\ref{thm:main}]
568
+ Take $K_2,H_2,a_2,b_2$ from Theorem~\ref{thm:input}. Apply
569
+ Lemma~\ref{lem:binary} with $d=[K_2:\F_2]\ge1$ and then
570
+ Proposition~\ref{prop:separation}. It gives the group
571
+ $G_D=(\bigoplus_{H_2}C_3)\rtimes H_2$ and a projection $P$
572
+ of size $d+1$ whose binary reduction factors through $d$ columns.
573
+ Its trace is $d+\theta$, where
574
+ \[
575
+ \theta=\frac13\left(\frac23\right)^{|S|}>0,
576
+ \qquad D=3^{1+|S|}.
577
+ \]
578
+ The odd integer $D$ clears the coefficients of $P$. Choose
579
+ $k\ge1$ with $q=2^k\equiv1\pmod D$.
580
+ Proposition~\ref{prop:criterion}, with $r=d$ and $m=d+1$,
581
+ produces $A\in\Mat_{2d+1}(\Z[G_D])$ with a rational group-ring
582
+ inverse and
583
+ \[
584
+ \log\det_{\N(G_D)}(T_A)=-\theta\log q.
585
+ \]
586
+ Since $q>1$ and $\theta>0$, this proves
587
+ \begin{equation}\label{eq:final-det}
588
+ 0<\det_{\N(G_D)}(T_A)=q^{-\theta}<1.
589
+ \end{equation}
590
+ With $n=2d+1$, Equation~\eqref{eq:criterion-integral} reads
591
+ \begin{equation}\label{eq:final-integral}
592
+ \int_{(0,\infty)}\log t\,d\mu_A(t)
593
+ =-\frac{2\theta\log q}{2d+1}<0.
594
+ \end{equation}
595
+ It is finite because of the spectral bounds in
596
+ Proposition~\ref{prop:criterion}. Finally, a finite generating
597
+ set of $H_2$ together with $z_1$ generates $G_D$, since
598
+ $z_h=hz_1h^{-1}$. Thus $G_D$ is finitely generated.
599
+ \end{proof}
600
+
601
+ The target group differs from the companion's group and contains
602
+ the cyclic coordinates of order three. The construction has a
603
+ finite negative logarithmic determinant and no zero spectral mass;
604
+ it is a failure of the asserted lower bound, not of determinant
605
+ class. Applying the sofic determinant bound of
606
+ \cite[Theorem 5]{ElekSzabo2005} to the positive integral matrix
607
+ $A^*A$ proves that $G_D$ is not sofic. This last implication is an
608
+ external consequence, not an ingredient in constructing $A$.
609
+
610
+ \begingroup
611
+ \raggedright
612
+ \bibliographystyle{plain}
613
+ \bibliography{references}
614
+ \endgroup
615
+ \end{document}
preprints/A-Counterexample-to-the-Group-Ring-Determinant-Conjecture-September-23-2026/build/references.bib ADDED
@@ -0,0 +1,108 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ @book{Luck2002,
2
+ author = {Wolfgang L{\"u}ck},
3
+ title = {{$L^2$-Invariants: Theory and Applications to Geometry and $K$-Theory}},
4
+ series = {Ergebnisse der Mathematik und ihrer Grenzgebiete. 3. Folge},
5
+ volume = {44},
6
+ publisher = {Springer},
7
+ year = {2002},
8
+ doi = {10.1007/978-3-662-04687-6}
9
+ }
10
+
11
+ @article{ElekSzabo2005,
12
+ author = {G{\'a}bor Elek and Endre Szab{\'o}},
13
+ title = {Hyperlinearity, essentially free actions and {$L^2$}-invariants.
14
+ {The} sofic property},
15
+ journal = {Mathematische Annalen},
16
+ volume = {332},
17
+ pages = {421--441},
18
+ year = {2005},
19
+ doi = {10.1007/s00208-005-0640-8}
20
+ }
21
+
22
+ @article{FK1952,
23
+ author = {Bent Fuglede and Richard V. Kadison},
24
+ title = {Determinant theory in finite factors},
25
+ journal = {Annals of Mathematics},
26
+ series = {2},
27
+ volume = {55},
28
+ number = {3},
29
+ pages = {520--530},
30
+ year = {1952},
31
+ doi = {10.2307/1969645}
32
+ }
33
+
34
+ @misc{CharacteristicTwo,
35
+ author = {{OpenAI}},
36
+ title = {{A Counterexample to Kaplansky's Direct-Finiteness Conjecture in Characteristic Two}},
37
+ howpublished = {OpenAI Math Release preprint
38
+ \href{https://github.com/openai/math/blob/main/preprints/A-Counterexample-to-Kaplanskys-Direct-Finiteness-Conjecture-in-Characteristic-Two-September-23-2026/paper.pdf}{OAI:A-Counterexample-to-Kaplanskys-Direct-Finiteness-Conjecture-in-Characteristic-Two-September-23-2026}},
39
+ year = {2026},
40
+ note = {Theorem 1.1 and Section 6}
41
+ }
42
+
43
+ @misc{Kammeyer2026,
44
+ author = {Holger Kammeyer},
45
+ title = {A counterexample to the determinant approximation conjecture},
46
+ year = {2026},
47
+ eprint = {2609.15567},
48
+ howpublished = {\href{https://arxiv.org/abs/2609.15567v1}{arXiv:2609.15567v1}},
49
+ archivePrefix = {arXiv},
50
+ primaryClass = {math.GR},
51
+ note = {Version 1, September 14, 2026},
52
+ url = {https://arxiv.org/abs/2609.15567v1}
53
+ }
54
+
55
+ @article{DicksSchick2002,
56
+ author = {Warren Dicks and Thomas Schick},
57
+ title = {The spectral measure of certain elements of the complex group ring of a wreath product},
58
+ journal = {Geometriae Dedicata},
59
+ volume = {93},
60
+ pages = {121--137},
61
+ year = {2002},
62
+ doi = {10.1023/A:1020381532489},
63
+ eprint = {math/0107145},
64
+ archivePrefix = {arXiv},
65
+ url = {https://arxiv.org/abs/math/0107145}
66
+ }
67
+
68
+ @article{LehnerNeuhauserWoess2008,
69
+ author = {Franz Lehner and Markus Neuhauser and Wolfgang Woess},
70
+ title = {On the spectrum of lamplighter groups and percolation clusters},
71
+ journal = {Mathematische Annalen},
72
+ volume = {342},
73
+ number = {1},
74
+ pages = {69--89},
75
+ year = {2008},
76
+ doi = {10.1007/s00208-008-0222-7},
77
+ eprint = {0712.3135},
78
+ archivePrefix = {arXiv},
79
+ url = {https://arxiv.org/abs/0712.3135}
80
+ }
81
+
82
+ @article{deLaHarpeSkandalis1984,
83
+ author = {de la Harpe, Pierre and Skandalis, Georges},
84
+ title = {D\'eterminant associ\'e \`a une trace sur une alg\`ebre de {Banach}},
85
+ journal = {Annales de l'Institut Fourier},
86
+ volume = {34},
87
+ number = {1},
88
+ pages = {241--260},
89
+ year = {1984},
90
+ doi = {10.5802/aif.958},
91
+ url = {https://www.numdam.org/articles/10.5802/aif.958/}
92
+ }
93
+
94
+ @article{Schick2001,
95
+ author = {Thomas Schick},
96
+ title = {{$L^2$}-determinant class and approximation of {$L^2$}-{Betti} numbers},
97
+ journal = {Transactions of the American Mathematical Society},
98
+ volume = {353},
99
+ number = {8},
100
+ pages = {3247--3265},
101
+ year = {2001},
102
+ doi = {10.1090/S0002-9947-01-02699-X},
103
+ eprint = {math/9807032},
104
+ archivePrefix = {arXiv},
105
+ url = {https://arxiv.org/abs/math/9807032v2},
106
+ note = {With the appended erratum in
107
+ \href{https://arxiv.org/abs/math/9807032v2}{arXiv:math/9807032v2}}
108
+ }
preprints/A-Counterexample-to-the-Group-Ring-Determinant-Conjecture-September-23-2026/paper.pdf ADDED
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+ oid sha256:3524b6f2390f17d5af1f06d76bfa0a6560cbdc3cb6d1d316fcdf17a715d0de40
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+ size 311036
preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/README.md ADDED
@@ -0,0 +1,20 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ # [A Counterexample to the Infinite Matroid Packing/Covering Conjecture](paper.pdf)
2
+
3
+ **Author:** OpenAI
4
+
5
+ **Date:** September 24, 2026
6
+
7
+ ## Citation
8
+
9
+ To cite this manuscript:
10
+
11
+ ```bibtex
12
+ @misc{OAI:A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026,
13
+ author = {{OpenAI}},
14
+ title = {{A Counterexample to the Infinite Matroid Packing/Covering Conjecture}},
15
+ howpublished = {OpenAI Math Release preprint
16
+ \href{https://github.com/openai/math/blob/main/preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/paper.pdf}{OAI:A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026}},
17
+ year = {2026}
18
+ }
19
+ ```
20
+
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+ \usepackage[colorlinks=true,linkcolor=blue!45!black,citecolor=blue!45!black,urlcolor=blue!45!black]{hyperref}
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+ \hypersetup{pdftitle={A Counterexample to the Infinite Matroid Packing/Covering Conjecture},pdfauthor={OpenAI}}
59
+ \newtheorem{theorem}{Theorem}[section]
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+ \newtheorem{proposition}[theorem]{Proposition}
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+ \newtheorem{lemma}[theorem]{Lemma}
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+ \newtheorem{corollary}[theorem]{Corollary}
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+ \numberwithin{equation}{section}
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+ \DeclareMathOperator{\cl}{cl}
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+ \setlist{itemsep=3pt,topsep=5pt}
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+ \title{A Counterexample to the Infinite Matroid\newline Packing/Covering Conjecture}
71
+ \author{OpenAI}
72
+ \date{September 24, 2026}
73
+ \begin{document}
74
+ \maketitle
75
+ \begin{abstract}
76
+ We construct in ZFC two self-dual partitional matroids on a countably infinite
77
+ common ground set that admit neither a packing/covering partition nor an
78
+ intersection witness. This disproves the unrestricted infinite matroid
79
+ packing/covering and intersection conjectures and answers Jo\'o's question
80
+ for two partitional matroids negatively. The examples are neither finitary
81
+ nor cofinitary.
82
+ \end{abstract}
83
+ \begingroup
84
+ \small
85
+ \tableofcontents
86
+ \endgroup
87
+ \clearpage
88
+ \input{sections/01-introduction}
89
+ \input{sections/02-matroids}
90
+ \input{sections/03-filters}
91
+ \input{sections/04-local-bases}
92
+ \input{sections/05-assembly}
93
+ \input{sections/06-counterexample}
94
+ \input{sections/07-consequences}
95
+ \begingroup\small
96
+ \bibliographystyle{plain}
97
+ \bibliography{references}
98
+ \endgroup
99
+ \end{document}
preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/build/references.bib ADDED
@@ -0,0 +1,83 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ @article{BDKPW2013,
2
+ author = {Bruhn, Henning and Diestel, Reinhard and Kriesell, Matthias and Pendavingh, Rudi and Wollan, Paul},
3
+ title = {Axioms for infinite matroids},
4
+ journal = {Advances in Mathematics},
5
+ volume = {239},
6
+ year = {2013},
7
+ pages = {18--46},
8
+ doi = {10.1016/j.aim.2013.01.011}
9
+ }
10
+
11
+ @article{BowlerCarmesin2015,
12
+ author = {Bowler, Nathan and Carmesin, Johannes},
13
+ title = {Matroid intersection, base packing and base covering for infinite matroids},
14
+ journal = {Combinatorica},
15
+ volume = {35},
16
+ number = {2},
17
+ year = {2015},
18
+ pages = {153--180},
19
+ doi = {10.1007/s00493-014-2953-2},
20
+ note = {Numbered locators refer to the \href{https://www.math.uni-hamburg.de/spag/dm/papers/PackingCovering.pdf}{author version dated 25 June 2014}}
21
+ }
22
+
23
+ @article{BowlerGeschke2016,
24
+ author = {Bowler, Nathan and Geschke, Stefan},
25
+ title = {Self-dual uniform matroids on infinite sets},
26
+ journal = {Proceedings of the American Mathematical Society},
27
+ volume = {144},
28
+ number = {2},
29
+ year = {2016},
30
+ pages = {459--471},
31
+ doi = {10.1090/proc/12667},
32
+ note = {Numbered locators refer to the \href{https://www.math.uni-hamburg.de/home/geschke/papers/UniformMatroid7.pdf}{author version dated 6 October 2014}}
33
+ }
34
+
35
+ @misc{GollinJoo2025,
36
+ author = {Gollin, J. Pascal and Jo{\'o}, Attila},
37
+ title = {Wild generalised truncation of infinite matroids},
38
+ year = {2025},
39
+ note = {\href{https://arxiv.org/abs/2504.05064v1}{arXiv:2504.05064v1}, 7 April 2025}
40
+ }
41
+
42
+ @article{Joo2024Packing,
43
+ author = {Jo{\'o}, Attila},
44
+ title = {On the packing/covering conjecture of infinite matroids},
45
+ journal = {Israel Journal of Mathematics},
46
+ volume = {261},
47
+ number = {2},
48
+ year = {2024},
49
+ pages = {765--790},
50
+ doi = {10.1007/s11856-023-2595-4}
51
+ }
52
+
53
+ @article{Joo2021Partitional,
54
+ author = {Jo{\'o}, Attila},
55
+ title = {Intersection of a partitional and a general infinite matroid},
56
+ journal = {Discrete Mathematics},
57
+ volume = {344},
58
+ number = {9},
59
+ year = {2021},
60
+ pages = {112514},
61
+ doi = {10.1016/j.disc.2021.112514}
62
+ }
63
+
64
+ @article{Joo2021Countable,
65
+ author = {Jo{\'o}, Attila},
66
+ title = {Proof of {Nash-Williams}' intersection conjecture for countable matroids},
67
+ journal = {Advances in Mathematics},
68
+ volume = {380},
69
+ year = {2021},
70
+ pages = {107608},
71
+ doi = {10.1016/j.aim.2021.107608}
72
+ }
73
+
74
+ @article{AharoniZiv1998,
75
+ author = {Aharoni, Ron and Ziv, Ran},
76
+ title = {The intersection of two infinite matroids},
77
+ journal = {Journal of the London Mathematical Society},
78
+ volume = {58},
79
+ number = {3},
80
+ year = {1998},
81
+ pages = {513--525},
82
+ doi = {10.1112/S0024610798006723}
83
+ }
preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/build/sections/01-introduction.tex ADDED
@@ -0,0 +1,202 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Introduction}\label{sec:introduction}
2
+
3
+ A \emph{packing} of a family of matroids on a common ground set is a choice
4
+ of pairwise disjoint spanning sets, one for each matroid. A \emph{covering}
5
+ is a choice of independent sets, one for each matroid, whose union is the
6
+ ground set. The infinite matroid packing/covering conjecture asks whether
7
+ every family admits a partition of the ground set on which these two
8
+ requirements can be satisfied in the following complementary senses.
9
+
10
+ Throughout, matroids are standard infinite matroids, with the maximal
11
+ extension axiom recalled in Section~\ref{sec:matroids}. For a matroid $M$
12
+ on $E$ and $X\subseteq E$, write $M\!\upharpoonright X$ for restriction
13
+ and
14
+ \[
15
+ M.X:=M/(E\setminus X)=(M^*\!\upharpoonright X)^*
16
+ \]
17
+ for contraction onto $X$. A set is spanning if its closure is the whole
18
+ ground set. A \emph{packing/covering partition} for $(M_i:i\in\Theta)$ is
19
+ a partition $E=P\dot\cup C$ together with sets $S_i\subseteq P$ and
20
+ $I_i\subseteq C$ such that
21
+ \begin{align*}
22
+ S_i\cap S_j&=\varnothing &&(i\ne j),\\
23
+ \cl_{M_i\upharpoonright P}(S_i)&=P &&(i\in\Theta),\\
24
+ I_i&\text{ is independent in }M_i.C &&(i\in\Theta),\\
25
+ \bigcup_{i\in\Theta}I_i&=C.
26
+ \end{align*}
27
+ Bowler and Carmesin formulated the assertion that every set-indexed family
28
+ has such a partition and established its relationship with infinite
29
+ matroid intersection~\cite[Conjecture~1.3 and Corollary~3.9]{BowlerCarmesin2015}. We give a counterexample
30
+ with two matroids.
31
+
32
+ \begin{theorem}\label{thm:main}
33
+ In ZFC, there exist a countably infinite set $E$ and two infinite matroids
34
+ $M_0,M_1$ on $E$ such that $M_i^*=M_i$ on the same labelled ground set for
35
+ $i=0,1$, and
36
+ \[
37
+ I_0\cup I_1\ne E
38
+ \quad\text{for every independent }I_0\text{ in }M_0
39
+ \text{ and independent }I_1\text{ in }M_1.
40
+ \]
41
+ The pair $(M_0,M_1)$ has no packing/covering partition. Consequently, the
42
+ infinite matroid packing/covering conjecture is false.
43
+ \end{theorem}
44
+
45
+ The last conclusion needs a separate argument: failure of a covering of
46
+ $E$ alone does not rule out a mixed partition. For a self-dual pair,
47
+ however, the spanning sets on $P$ and the independent sets in the
48
+ contractions onto $C$ give disjoint spanning sets on $E$. Their complements
49
+ are an independent covering. We prove this implication in
50
+ Section~\ref{sec:matroids} before constructing the counterexample.
51
+
52
+ \subsection*{Context and the local construction}
53
+
54
+ The axioms of Bruhn, Diestel, Kriesell, Pendavingh and
55
+ Wollan~\cite{BDKPW2013} provide an infinite matroid theory with restriction,
56
+ contraction and duality. In particular, independent sets must extend to
57
+ maximal independent sets inside \emph{every} prescribed subset of the
58
+ ground set. This condition is a central part of our construction.
59
+
60
+ A matroid is \emph{uniform} if replacing any element of any basis by any
61
+ element outside that basis again gives a basis. Bowler and
62
+ Geschke~\cite[Theorem~6 and the proof of Theorem~15]{BowlerGeschke2016} developed a basis criterion for infinite
63
+ uniform matroids and constructed countable self-dual examples under
64
+ Martin's axiom for countable partially ordered sets, and hence under the
65
+ continuum hypothesis. Their criterion combines an
66
+ antichain of bases, invariance under balanced finite changes, and a basis
67
+ existence condition for intervals of subsets. Our assembly also uses the
68
+ complementary interval-recursion pattern of their Lemma~12, while
69
+ verifying the full independent-set axioms directly.
70
+
71
+ Bowler and Geschke left open whether an infinite self-dual uniform matroid
72
+ can be constructed in ZFC. Even without self-duality, ZFC existence of a
73
+ uniform matroid of infinite rank and corank is recorded as open by Gollin
74
+ and Jo\'o~\cite[Section~1]{GollinJoo2025}.
75
+
76
+ Our local construction gives a self-dual uniform matroid $Q$ on a
77
+ countable set in ZFC, with every basis and its complement infinite.
78
+ It therefore answers both of these existence questions affirmatively.
79
+ Its bases satisfy an additional ordinal inequality that obstructs
80
+ independent coverings when copies of $Q$ are placed along a doubly
81
+ infinite path. The two matroids in Theorem~\ref{thm:main} are countably
82
+ infinite direct sums of these copies. In Jo\'o's terminology, a direct sum
83
+ of uniform matroids is \emph{partitional}. His definition of uniformity is
84
+ equivalent to requiring every subset to be independent or spanning
85
+ \cite[Definition~1.2 and Proposition~2.2]{Joo2021Partitional}, the property
86
+ proved for $Q$ in Remark~\ref{rem:uniform-local}. Thus both matroids in our
87
+ pair are partitional. This distinction matters: Jo\'o proved an intersection
88
+ theorem for an arbitrary infinite matroid paired with a direct sum of
89
+ \emph{finitely many} uniform matroids, and asked whether intersection holds
90
+ for two partitional matroids on a common countable ground set
91
+ \cite[Theorem~1.4 and Question~1.5]{Joo2021Partitional}.
92
+
93
+ For matroids $M,N$ on a common ground set $E$, the pair \emph{satisfies
94
+ intersection} if there is a set $J$ independent in both matroids and a
95
+ partition $J=J_M\dot\cup J_N$ such that
96
+ \[
97
+ \cl_M(J_M)\cup\cl_N(J_N)=E.
98
+ \]
99
+ The unrestricted infinite Matroid Intersection Conjecture asserts that
100
+ every pair of matroids on a common, possibly infinite, ground set satisfies this
101
+ property~\cite[Definition~3.5 and Section~7]{BowlerCarmesin2015}.
102
+
103
+ \begin{corollary}\label{cor:intersection}
104
+ The same pair $(M_0,M_1)$ constructed in Theorem~\ref{thm:main} consists of
105
+ partitional matroids and does not satisfy intersection. More explicitly,
106
+ for every set $J$ independent in both $M_0$ and $M_1$ and every partition
107
+ $J=J_0\dot\cup J_1$,
108
+ \[
109
+ \cl_{M_0}(J_0)\cup\cl_{M_1}(J_1)\ne E.
110
+ \]
111
+ Consequently, the unrestricted infinite Matroid Intersection Conjecture is
112
+ false in ZFC. The pair also gives a negative ZFC answer to Jo\'o's
113
+ Question~1.5 for two partitional matroids on a common countable ground set.
114
+ \end{corollary}
115
+
116
+ \begin{proof}
117
+ Each $M_i$ is a direct sum of countably infinitely many copies of the uniform
118
+ matroid $Q$, so it is partitional. Bowler and Carmesin
119
+ \cite[Proposition~3.6]{BowlerCarmesin2015} prove that, for any matroids $M,N$
120
+ on the same ground set,
121
+ \[
122
+ (M,N)\text{ satisfies intersection}
123
+ \quad\Longleftrightarrow\quad
124
+ (M,N^*)\text{ has a packing/covering partition}.
125
+ \]
126
+ Apply this equivalence with $M=M_0$ and $N=M_1$. Since $M_1^*=M_1$ on the same labelled ground set,
127
+ the right-hand side concerns the identical pair $(M_0,M_1)$ and is false by
128
+ Theorem~\ref{thm:main}. Its common ground set is countable, so it also
129
+ satisfies the hypotheses of Jo\'o's question.
130
+ \end{proof}
131
+
132
+ Bowler and Carmesin also formulated separate Covering and Packing
133
+ conjectures. Their universal equivalences imply that both conjectures are
134
+ false in ZFC; Section~\ref{sec:separate-consequences} gives the precise
135
+ formulations and deduction. This consequence concerns universal statements
136
+ about matroid families and does not identify their witnessing families
137
+ with the pair $(M_0,M_1)$.
138
+
139
+ The examples are neither finitary nor cofinitary. Here a matroid is
140
+ \emph{finitary} if a set is independent whenever all its finite subsets
141
+ are independent, and \emph{cofinitary} if its dual is finitary. Nash-Williams' original intersection conjecture concerned finitary
142
+ matroids; Aharoni and Ziv~\cite{AharoniZiv1998} gave an early published
143
+ formulation. Jo\'o proved intersection for two finitary matroids on a countable
144
+ ground set~\cite[Theorem~1.3]{Joo2021Countable}.
145
+ His subsequent packing/covering theorem allows every set-indexed family
146
+ on a countable ground set whose members are direct sums of finitary and
147
+ cofinitary matroids~\cite[Theorem~1.2]{Joo2024Packing}.
148
+ The examples here have no nonempty finitary or cofinitary direct summand,
149
+ as we show in Section~\ref{sec:counterexample}, so they lie outside this
150
+ mixed direct-sum class. Countability of the ground set is distinct from
151
+ these structural hypotheses; the present result concerns unrestricted
152
+ infinite matroids and does not refute Nash-Williams' original finitary
153
+ conjecture.
154
+
155
+ \subsection*{Proof overview}
156
+
157
+ We first construct an ultrafilter $\mathcal U$ on a countable set $D$ and
158
+ an ordinal-valued function $\rho$ on its members. Call a subset of $D$
159
+ \emph{large} if it belongs to $\mathcal U$. This auxiliary ordinal rank, distinct from matroid rank, satisfies
160
+ $\rho(X)\ge\rho(Y)$ whenever $X\subseteq Y$ are large. On two labelled copies $L,R$ of $D$, we construct
161
+ a self-dual matroid $Q$ with the following property: if $B$ is a basis
162
+ and its slice $B_L\subseteq D$ is large, then $D\setminus B_R$ is large
163
+ and
164
+ \[
165
+ \rho(B_L)>\rho(D\setminus B_R).
166
+ \]
167
+ This is the property used at the end of the proof. To build the pair,
168
+ join consecutive integer vertices by \emph{bundles}, each a labelled
169
+ copy of $D$, and place $Q$ on the two incident bundles at each vertex.
170
+ Its $L$-coordinate points toward the central bundle between $-1$ and $0$,
171
+ and its $R$-coordinate points outward. The copies at even and odd vertices
172
+ form $M_0$ and $M_1$, respectively. In a putative independent covering, one starts with the large side of a
173
+ central bundle and follows the path outward. Each successive copy of
174
+ $Q$ strictly decreases the ordinal rank, an impossibility.
175
+
176
+ Most of the proof constructs $Q$. Partition $D$ into rapidly growing
177
+ finite blocks. The first ideal consists of subsets whose proportions
178
+ in these blocks tend to zero. Within each equivalence class modulo this
179
+ ideal, we define real-valued probes of a subset; a half-open interval
180
+ condition on their lower or upper limits selects the bases. Finite
181
+ changes shift these limits by their net cardinality, making basis
182
+ exchange immediate. A separate interpolation argument supplies bases
183
+ between suitable endpoints, including endpoints with infinite limits.
184
+ This argument is the key to maximal extension.
185
+
186
+ A second, larger ideal permits the insertion of sets that preserve the
187
+ ordinal inequalities while separating previously chosen classes.
188
+ Independent binary columns supply these separating sets simultaneously
189
+ for fewer than continuum many requirements. We then address every
190
+ interval of subsets in a transfinite recursion, inserting complementary
191
+ classes of bases when necessary. At each stage there are fewer than
192
+ continuum many earlier requirements; no regularity assumption on the
193
+ continuum is used.
194
+
195
+ Section~\ref{sec:filters} constructs the two ideals, the ultrafilter, the
196
+ rank and the simultaneous reservations. Section~\ref{sec:local-bases}
197
+ proves the interpolation properties within a single class.
198
+ Section~\ref{sec:assembly} assembles the classes and proves all the
199
+ matroid axioms, including maximal extension.
200
+ Section~\ref{sec:counterexample} places $Q$ along the path and completes
201
+ the ordinal descent argument. Section~\ref{sec:separate-consequences}
202
+ derives the separate universal Covering and Packing consequences.
preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/build/sections/02-matroids.tex ADDED
@@ -0,0 +1,119 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Matroids and the self-dual reduction}\label{sec:matroids}
2
+
3
+ We first record the infinite-matroid conventions and explain why, for a
4
+ self-dual pair, it suffices to rule out an independent covering of the
5
+ whole ground set. This reduction is essential: a mixed packing/covering
6
+ partition need not be a packing or a covering on the whole set.
7
+
8
+ \subsection{Independence, closure, and duality}
9
+
10
+ An infinite matroid on a set $F$ is a family $\mathcal I\subseteq 2^F$
11
+ satisfying the following axioms
12
+ \cite[Section~1.1]{BDKPW2013}:
13
+ \begin{description}
14
+ \item[(I1)] $\varnothing\in\mathcal I$.
15
+ \item[(I2)] Every subset of a member of $\mathcal I$ belongs to $\mathcal I$.
16
+ \item[(I3)] If $I\in\mathcal I$ is not inclusion-maximal and
17
+ $B\in\mathcal I$ is inclusion-maximal, there is an element
18
+ $e\in B\setminus I$ such that $I\cup\{e\}\in\mathcal I$.
19
+ \item[(IM)] For every $I\in\mathcal I$ and $I\subseteq Y\subseteq F$,
20
+ the family $\{J\in\mathcal I:I\subseteq J\subseteq Y\}$ has an
21
+ inclusion-maximal member.
22
+ \end{description}
23
+ The inclusion-maximal independent sets are the \emph{bases}. In
24
+ particular, (IM) requires maximal extensions inside every subset, not
25
+ only inside $F$.
26
+
27
+ For a matroid $N=(F,\mathcal I)$ and $X\subseteq F$, its closure is
28
+ \[
29
+ \operatorname{cl}_N(X)=X\cup
30
+ \{e\in F:\text{there is an independent }I\subseteq X
31
+ \text{ with }I\cup\{e\}\text{ dependent}\}.
32
+ \]
33
+ This operator is extensive, monotone, and idempotent
34
+ \cite[Theorem~4.2]{BDKPW2013}. A set $S$ is \emph{spanning} if
35
+ $\operatorname{cl}_N(S)=F$.
36
+ Restrictions are matroids, and the complements of the bases of $N$
37
+ are the bases of its dual $N^*$
38
+ \cite[Theorems~3.1 and~3.4]{BDKPW2013}. We use
39
+ \[
40
+ N.X=N/(F\setminus X)=(N^*\!\upharpoonright X)^*
41
+ \]
42
+ for contraction onto $X$. Self-duality will always mean the equality
43
+ $N=N^*$ on the same labeled ground set.
44
+
45
+ \begin{lemma}\label{lem:closure-duality}
46
+ Let $N$ be an infinite matroid on $F$.
47
+ \begin{enumerate}
48
+ \item If $S\subseteq X\subseteq F$, then
49
+ \[
50
+ \operatorname{cl}_{N\upharpoonright X}(S)
51
+ =\operatorname{cl}_N(S)\cap X.
52
+ \]
53
+ \item A subset $S\subseteq F$ is spanning if and only if it contains
54
+ a basis of $N$.
55
+ \item A subset $S\subseteq F$ is spanning in $N$ if and only if
56
+ $F\setminus S$ is independent in $N^*$.
57
+ \end{enumerate}
58
+ \end{lemma}
59
+ \begin{proof}
60
+ The first assertion follows directly from the closure definition:
61
+ for $e\in X$, independence of sets contained in $S\cup\{e\}$ is
62
+ the same in $N$ and in its restriction to $X$.
63
+
64
+ For the second, use (IM) to take a maximal independent subset $B$ of
65
+ $S$. For every $e\in S\setminus B$, the set $B\cup\{e\}$ is
66
+ dependent, so $S\subseteq\operatorname{cl}_N(B)$. Monotonicity and
67
+ idempotence therefore give
68
+ \[
69
+ \operatorname{cl}_N(B)=\operatorname{cl}_N(S).
70
+ \]
71
+ If $S$ is spanning, so is $B$. An independent spanning set is a basis:
72
+ an independent extension by an element of its closure would contradict
73
+ the defining independent witness for closure. Conversely, a basis spans,
74
+ because adjoining any element outside it gives a dependent set; any set
75
+ containing a basis consequently spans.
76
+
77
+ If $S$ contains a basis $B$, then $F\setminus S$ is contained in
78
+ the dual basis $F\setminus B$. Conversely, extend an independent
79
+ $F\setminus S$ to a basis $B^*$ of $N^*$ using (IM).
80
+ The primal basis $F\setminus B^*$ is contained in $S$.
81
+ \end{proof}
82
+
83
+ \subsection{From a mixed partition to an independent covering}
84
+
85
+ \begin{lemma}\label{lem:selfdual-reduction}
86
+ Let $N_0,N_1$ be matroids on the same set $F$, with $N_i=N_i^*$
87
+ on the same labels. Suppose there is a partition
88
+ $F=P\mathbin{\dot\cup}C$, disjoint sets $S_0,S_1\subseteq P$
89
+ spanning $N_0\!\upharpoonright P,N_1\!\upharpoonright P$,
90
+ respectively, and independent sets $I_i$ of $N_i.C$ such that
91
+ $I_0\cup I_1=C$. Then $F$ can be covered by one independent set
92
+ of each of $N_0,N_1$.
93
+ \end{lemma}
94
+ \begin{proof}
95
+ Self-duality gives
96
+ \[
97
+ N_i.C=(N_i\!\upharpoonright C)^*.
98
+ \]
99
+ Thus $T_i=C\setminus I_i$ spans $N_i\!\upharpoonright C$ by
100
+ Lemma~\ref{lem:closure-duality}. Also
101
+ $T_0\cap T_1=C\setminus(I_0\cup I_1)=\varnothing$.
102
+ Consequently the two sets
103
+ \[
104
+ A_i=S_i\cup T_i\qquad(i=0,1)
105
+ \]
106
+ are disjoint. The restriction-closure identity shows that
107
+ $P\subseteq\operatorname{cl}_{N_i}(S_i)$ and
108
+ $C\subseteq\operatorname{cl}_{N_i}(T_i)$, so $A_i$ spans the
109
+ full matroid $N_i$. Its complement $F\setminus A_i$ is independent
110
+ in $N_i^*=N_i$. Finally,
111
+ \[
112
+ (F\setminus A_0)\cup(F\setminus A_1)=F
113
+ \]
114
+ because $A_0\cap A_1=\varnothing$.
115
+ \end{proof}
116
+
117
+ We will construct a self-dual pair with no independent covering.
118
+ Lemma~\ref{lem:selfdual-reduction} will then exclude every mixed
119
+ packing/covering partition for that pair.
preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/build/sections/03-filters.tex ADDED
@@ -0,0 +1,278 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{An ultrafilter rank and simultaneous reservations}
2
+ \label{sec:filters}
3
+
4
+ We construct two tools on a countable set. The first is an ordinal-valued
5
+ function on an ultrafilter whose value can be increased while preserving
6
+ a prescribed lower bound on the set. The second supplies two disjoint
7
+ sets that meet each of fewer than continuum many prescribed sets in
8
+ positive upper block density. These two tools will allow us to choose bases
9
+ with an ordinal inequality while also separating them from all earlier
10
+ choices.
11
+
12
+ \subsection{Blocks, columns, and two ideals}
13
+
14
+ Let $\mathfrak c=2^{\aleph_0}$, also regarded as its initial ordinal.
15
+ For each integer $m\ge0$, let
16
+ \[
17
+ D_m=\{m\}\times\{0,1\}^{\{0,1\}^m},\qquad
18
+ D=\coprod_{m\ge0}D_m,\qquad w_m=|D_m|=2^{2^m}.
19
+ \]
20
+ Thus $D$ is countably infinite. The tags $m$ make its finite blocks
21
+ disjoint. Their sizes satisfy
22
+ \begin{equation}\label{eq:block-growth}
23
+ w_m\ge2\sum_{j<m}w_j\qquad(m\ge1).
24
+ \end{equation}
25
+ Indeed, equality holds for $m=1$. If the inequality holds for $m$, then
26
+ $2\sum_{j<m+1}w_j\le3w_m\le w_m^2=w_{m+1}$, since $w_m\ge4$.
27
+
28
+ The density-zero ideal on $D$ is
29
+ \[
30
+ \mathcal J=\left\{X\subseteq D:
31
+ \frac{|X\cap D_m|}{w_m}\longrightarrow0\right\}.
32
+ \]
33
+ An ideal is a family closed under taking subsets and finite unions;
34
+ we call a set \emph{positive} for the ideal if it does not belong to it.
35
+ The displayed family is a proper ideal containing all finite sets.
36
+
37
+ Let $L$ and $R$ be labelled copies of $D$, and write
38
+ $E_0=L\mathbin{\dot\cup}R$. For $X\subseteq E_0$, its two slices,
39
+ viewed as subsets of $D$, are denoted by $X_L$ and $X_R$.
40
+ When writing lifts, we identify $E_0$ with $D\times\{L,R\}$.
41
+ Write $W_m$ for the union of the two copies of $D_m$.
42
+ The ideal $\mathcal J_0$ on $E_0$ consists of the sets whose two slices
43
+ belong to $\mathcal J$. Equivalently,
44
+ \[
45
+ X\in\mathcal J_0
46
+ \quad\Longleftrightarrow\quad
47
+ \frac{|X\cap W_m|}{|W_m|}\longrightarrow0.
48
+ \]
49
+ This equivalence follows because the doubled-block density is the
50
+ average of the two nonnegative slice densities. Complements are always
51
+ taken in the relevant ground set, $D$ or $E_0$.
52
+
53
+ \begin{lemma}[Independent columns]\label{lem:columns}
54
+ There are subsets $A_t,B_t,G_t$ of $D$, indexed by $t<\mathfrak c$,
55
+ with the following property. For any $r$ distinct columns from these
56
+ three families and any prescribed membership pattern on them, the
57
+ proportion of that pattern in $D_m$ is exactly $2^{-r}$ for all
58
+ sufficiently large $m$.
59
+ \end{lemma}
60
+
61
+ \begin{proof}
62
+ Assign distinct infinite binary strings to all the columns; this is
63
+ possible because $3\mathfrak c=\mathfrak c$. For a column with string
64
+ $h$, put $(m,f)$ in that column precisely when
65
+ $f(h\upharpoonright m)=1$.
66
+ The prefixes of any fixed finite list of distinct strings are distinct
67
+ for all sufficiently large $m$. Prescribing the values of $f$ at these
68
+ $r$ arguments leaves $2^{2^m-r}$ functions among the $2^{2^m}$ choices
69
+ in $D_m$, proving the assertion.
70
+ \end{proof}
71
+
72
+ We need a larger ideal in addition to $\mathcal J$. Define
73
+ \begin{equation}\label{eq:larger-ideal}
74
+ \mathcal K=\left\{X\subseteq D:
75
+ X\cap\bigcap_{t\in F}A_t\in\mathcal J
76
+ \text{ for some finite }F\subseteq\mathfrak c\right\},
77
+ \end{equation}
78
+ where an empty intersection is $D$. This is the ideal generated by
79
+ $\mathcal J$ and the complements $A_t^c$. To see the equivalence, split
80
+ $X$ into its intersection with the positive $A$-columns in
81
+ \eqref{eq:larger-ideal} and its remaining part, which is covered by
82
+ their complements. In particular $\mathcal J\subseteq\mathcal K$.
83
+ Lemma~\ref{lem:columns} shows that $D\notin\mathcal K$, so this ideal
84
+ is proper.
85
+
86
+ We will repeatedly use the following consequence. A consistent finite
87
+ pattern prescribing positive membership in $A$-columns and arbitrary
88
+ signs in $G$-columns is $\mathcal K$-positive. Intersecting such a pattern
89
+ with any further finitely many positive $A$-columns still gives a
90
+ pattern with a fixed positive eventual density, so
91
+ \eqref{eq:larger-ideal} excludes membership in $\mathcal K$.
92
+
93
+ Write $X\subseteq_{\mathcal K}Y$ if $X\setminus Y\in\mathcal K$.
94
+ On $E_0$, let $\mathcal K_0$ be the ideal of sets whose two slices
95
+ belong to $\mathcal K$. Thus $\mathcal J_0\subseteq\mathcal K_0$.
96
+ The distinction between these ideals matters: changes in
97
+ $\mathcal K_0$ will preserve an ordinal condition, whereas differences
98
+ positive for $\mathcal J_0$ will keep the resulting bases incomparable.
99
+
100
+ \subsection{The ultrafilter and its ordinal rank}
101
+
102
+ An ultrafilter $\mathcal U$ on $D$ is a proper filter that contains
103
+ exactly one of $X$ and $D\setminus X$ for every $X\subseteq D$.
104
+
105
+ \begin{lemma}\label{lem:ultrafilter}
106
+ There is an ultrafilter $\mathcal U$ on $D$ disjoint from $\mathcal K$,
107
+ containing every $G_t$, and satisfying
108
+ \begin{equation}\label{eq:finitely-many-columns}
109
+ X\in\mathcal U\quad\Longrightarrow\quad
110
+ \{t<\mathfrak c:X\subseteq_{\mathcal K}G_t\}
111
+ \text{ is finite}.
112
+ \end{equation}
113
+ \end{lemma}
114
+
115
+ \begin{proof}
116
+ Call $Z\subseteq D$ forbidden if it is contained modulo $\mathcal K$
117
+ in infinitely many of the $G_t$. Require a filter to contain all
118
+ complements of members of $\mathcal K$, all $G_t$, and all complements
119
+ of forbidden sets. We verify the finite-intersection property.
120
+
121
+ Combine the finitely many $\mathcal K$-small exclusions into one set
122
+ $N\in\mathcal K$. Let $F$ be the finite set of required positive
123
+ $G$-indices, and let $Z_1,\ldots,Z_q$ be the forbidden sets to exclude.
124
+ For each $j$, choose an index $t_j$ such that
125
+ $Z_j\setminus G_{t_j}\in\mathcal K$, with the $t_j$ distinct and
126
+ outside $F$. Each $Z_j$ has infinitely many witnessing indices, so
127
+ these choices are possible. The pattern
128
+ \[
129
+ P=\bigcap_{t\in F}G_t\cap\bigcap_{j=1}^qG_{t_j}^c
130
+ \]
131
+ is $\mathcal K$-positive. Moreover
132
+ $P\cap Z_j\subseteq Z_j\setminus G_{t_j}\in\mathcal K$.
133
+ It follows that
134
+ \[
135
+ P\setminus\left(N\cup\bigcup_{j=1}^qZ_j\right)
136
+ \]
137
+ is still $\mathcal K$-positive: otherwise $P$ would be a finite union
138
+ of members of $\mathcal K$. This nonempty set lies in the required
139
+ finite intersection. Extend the resulting proper filter to an
140
+ ultrafilter by the ultrafilter lemma. It contains no member of
141
+ $\mathcal K$ and no forbidden set, as required.
142
+ \end{proof}
143
+
144
+ Fix such an ultrafilter. Call its members \emph{large} and its
145
+ nonmembers \emph{small}. Small in this sense does not mean membership
146
+ in either ideal. Every large set is $\mathcal J$-positive, and every
147
+ complement of a $\mathcal K$-set is large.
148
+
149
+ List all large subsets of $D$ as $(F_\xi)_{\xi<\mathfrak c}$,
150
+ allowing repetitions if needed. For a large set $X$, define
151
+ \begin{equation}\label{eq:ordinal-rank}
152
+ \rho(X)=\min\{\xi<\mathfrak c:
153
+ F_\xi\subseteq_{\mathcal K}X\}.
154
+ \end{equation}
155
+ The set of indices is nonempty because $X$ occurs in the list.
156
+ This is an auxiliary ordinal rank, distinct from matroid rank.
157
+
158
+ \begin{lemma}[Rank invariance and monotonicity]\label{lem:rank}
159
+ If $X\triangle Y\in\mathcal K$, then $X$ is large if and only if $Y$
160
+ is large, and in that case $\rho(X)=\rho(Y)$.
161
+ If $X,Y$ are large and $X\subseteq_{\mathcal K}Y$, then
162
+ $\rho(X)\ge\rho(Y)$.
163
+ \end{lemma}
164
+
165
+ \begin{proof}
166
+ The complement of $X\triangle Y$ belongs to $\mathcal U$.
167
+ Intersecting it with either large set gives a large subset of the
168
+ other, proving invariance of largeness. The two sets have exactly the
169
+ same candidate indices in \eqref{eq:ordinal-rank}, proving rank
170
+ invariance. Finally, $F_\xi\subseteq_{\mathcal K}X$ and
171
+ $X\subseteq_{\mathcal K}Y$ imply
172
+ $F_\xi\subseteq_{\mathcal K}Y$ by closure of the ideal under finite
173
+ unions. Taking minima proves the last assertion.
174
+ \end{proof}
175
+
176
+ The next property supplies large sets of arbitrarily high rank inside
177
+ any interval whose lower endpoint is small and upper endpoint is
178
+ large.
179
+
180
+ \begin{lemma}[Rank-raising thinning]\label{lem:thinning}
181
+ Let $s\subseteq X\subseteq D$, with $s$ small and $X$ large, and let
182
+ $\gamma<\mathfrak c$. There is a large set $u$ such that
183
+ \[
184
+ s\subseteq u\subseteq X,\qquad \rho(u)>\gamma.
185
+ \]
186
+ \end{lemma}
187
+
188
+ \begin{proof}
189
+ For every $\xi\le\gamma$, the set
190
+ $Y_\xi=F_\xi\cap(X\setminus s)$ is large. By
191
+ \eqref{eq:finitely-many-columns}, it is contained modulo
192
+ $\mathcal K$ in only finitely many $G_t$.
193
+ The union of these finite sets of indices has cardinal at most
194
+ $\max(\aleph_0,|\gamma+1|)<\mathfrak c$. Choose $t$ outside that union
195
+ and put
196
+ \[
197
+ u=s\cup(X\cap G_t).
198
+ \]
199
+ Then $u$ is large and lies between $s$ and $X$.
200
+ If $F_\xi\subseteq_{\mathcal K}u$ for some $\xi\le\gamma$, then
201
+ \[
202
+ Y_\xi\setminus G_t
203
+ =F_\xi\cap X\cap s^c\cap G_t^c
204
+ \subseteq F_\xi\setminus u\in\mathcal K,
205
+ \]
206
+ contrary to the choice of $t$. Thus $\rho(u)>\gamma$.
207
+ \end{proof}
208
+
209
+ This counting argument does not require regularity of
210
+ $\mathfrak c$. For any fixed cardinal $\lambda<\mathfrak c$, a union
211
+ of $\lambda$ finite sets has cardinal at most
212
+ $\max(\lambda,\aleph_0)<\mathfrak c$. We will use this same estimate
213
+ at each stage of a recursion of length $\mathfrak c$.
214
+
215
+ \subsection{Two simultaneous reservations}
216
+
217
+ The ordinal rank is unchanged by $\mathcal K$-small changes. We now
218
+ show that such changes can nevertheless meet many prescribed sets
219
+ in a way that remains positive for the smaller ideal $\mathcal J$.
220
+ For $t<\mathfrak c$, define the following subsets of $E_0$, using the
221
+ same labels in both copies:
222
+ \[
223
+ H_{t,0}=(A_t^c\cap B_t^c)\times\{L,R\},\qquad
224
+ H_{t,1}=(A_t^c\cap B_t)\times\{L,R\}.
225
+ \]
226
+ They are disjoint, and both belong to $\mathcal K_0$ because their
227
+ slices lie in $A_t^c$.
228
+
229
+ \begin{lemma}[Simultaneous reservations]\label{lem:reservations}
230
+ Let $\mathscr S$ be a family of fewer than $\mathfrak c$ subsets of
231
+ $E_0$, each positive for $\mathcal J_0$. There is an index
232
+ $t<\mathfrak c$ such that
233
+ \[
234
+ S\cap H_{t,0}\notin\mathcal J_0
235
+ \quad\text{and}\quad
236
+ S\cap H_{t,1}\notin\mathcal J_0
237
+ \qquad(S\in\mathscr S).
238
+ \]
239
+ \end{lemma}
240
+
241
+ \begin{proof}
242
+ Fix first one $\mathcal J_0$-positive set $S$. Choose $\epsilon>0$
243
+ such that the proportion of $S$ in $W_m$ is at least $\epsilon$ for
244
+ infinitely many $m$. Call an index $t$ bad for $S$ if at least one
245
+ of $S\cap H_{t,0}$ and $S\cap H_{t,1}$ belongs to $\mathcal J_0$.
246
+ We prove that only finitely many indices are bad.
247
+
248
+ Choose any finite list of distinct bad indices $t_1,\ldots,t_q$, and
249
+ for each $i$ choose $k_i\in\{0,1\}$ with
250
+ $S\cap H_{t_i,k_i}\in\mathcal J_0$. Put $H_i=H_{t_i,k_i}$.
251
+ These cells use $2q$ distinct $A$- and $B$-columns. Avoiding $H_i$
252
+ allows three of the four membership patterns on its two columns.
253
+ Lemma~\ref{lem:columns} therefore gives $3^q$ avoiding patterns out of
254
+ $4^q$ equally frequent patterns in every sufficiently late block.
255
+ Duplicating the cells on the two copies does not change these proportions.
256
+ In particular,
257
+ \[
258
+ \frac{|W_m\setminus\bigcup_{i=1}^qH_i|}{|W_m|}
259
+ =\left(\frac34\right)^q
260
+ \]
261
+ for all sufficiently large $m$. Every point of $S\cap W_m$ either
262
+ avoids all these cells or lies in one of the failing intersections, so
263
+ \[
264
+ \frac{|S\cap W_m|}{|W_m|}
265
+ \le \left(\frac34\right)^q+
266
+ \sum_{i=1}^q\frac{|S\cap H_i\cap W_m|}{|W_m|}.
267
+ \]
268
+ Each summand tends to zero. Along the infinite subsequence on which
269
+ $S$ has density at least $\epsilon$, this gives
270
+ $\epsilon\le(3/4)^q$. Since $(3/4)^q\to0$, the size of any finite
271
+ list of bad indices is bounded. Hence only finitely many indices are bad.
272
+
273
+ For the family $\mathscr S$, take the union of these finite sets of
274
+ bad indices. Its cardinal is less than $\mathfrak c$ by the estimate
275
+ following Lemma~\ref{lem:thinning}. Any index outside that union
276
+ works simultaneously for every $S\in\mathscr S$. If the family is
277
+ empty, any index works.
278
+ \end{proof}
preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/build/sections/04-local-bases.tex ADDED
@@ -0,0 +1,332 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Bases within a density-zero class}\label{sec:local-bases}
2
+
3
+ We now construct families of candidate bases within one equivalence class
4
+ modulo $\mathcal J_0$. The purpose is twofold: balanced finite changes
5
+ must preserve the family, and intervals of subsets must contain or lie
6
+ on one side of a member of the family. The latter property will supply
7
+ maximal independent extensions in the eventual matroid.
8
+
9
+ Fix $T\subseteq E_0$ such that $T$ and $T^c$ are
10
+ $\mathcal J_0$-positive, and put
11
+ \[
12
+ \mathcal C(T)=\{X\subseteq E_0:X\triangle T\in\mathcal J_0\}.
13
+ \]
14
+ We use $T$ as the chosen representative, or \emph{prototype}, of this class.
15
+ Every member of $\mathcal C(T)$ and its complement are
16
+ $\mathcal J_0$-positive. Indeed, an ideal-small member, together with its
17
+ ideal-small symmetric difference from $T$, would make $T$ ideal-small;
18
+ the same argument applies to complements.
19
+
20
+ For $n\ge1$ and $m\ge0$, define
21
+ \begin{align}
22
+ V_n&=\bigcup_{m<n}W_m,\qquad c_n=|V_n|,\notag\\
23
+ p_n^T(X)&=|X\cap V_n|-|T\cap V_n|,\notag\\
24
+ d_m^T(X)&=\frac{|X\cap W_m|-|T\cap W_m|}{|W_m|},\notag\\
25
+ f_n^T(X)&=p_n^T(X)+c_n\left(
26
+ \sup_{m\ge n}d_m^T(X)+\inf_{m\ge n}d_m^T(X)\right).
27
+ \label{eq:probes}
28
+ \end{align}
29
+ These quantities are defined for $X\in\mathcal C(T)$. The prefix count
30
+ records a finite modification exactly once its affected blocks lie in
31
+ $V_n$. The tail extrema allow later-block changes to influence earlier
32
+ probes, and their sum changes sign when both $X$ and $T$ are complemented.
33
+ Write
34
+ \[
35
+ \ell_T(X)=\liminf_{n\to\infty}f_n^T(X),\qquad
36
+ h_T(X)=\limsup_{n\to\infty}f_n^T(X),
37
+ \]
38
+ allowing infinite values, and define two families
39
+ \begin{align}
40
+ \mathcal B^-(T)&=\{X\in\mathcal C(T):-1<\ell_T(X)\le0\},\notag\\
41
+ \mathcal B^+(T)&=\{X\in\mathcal C(T):0\le h_T(X)<1\}.
42
+ \label{eq:local-bases}
43
+ \end{align}
44
+ We call these the lower-limit and upper-limit rules, respectively.
45
+ In this section, a basis for a rule means a member of the indicated
46
+ family; no matroid is asserted yet.
47
+
48
+ \subsection{Probe estimates and continuity}
49
+
50
+ \begin{lemma}[Probe properties]\label{lem:probe-properties}
51
+ For $X,Y\in\mathcal C(T)$ the following statements hold.
52
+ \begin{enumerate}
53
+ \item $d_m^T(X)\to0$ and $p_n^T(X)/c_n\to0$.
54
+ \item If $X\subseteq Y$, then
55
+ \begin{equation}\label{eq:probe-monotone}
56
+ f_n^T(Y)-f_n^T(X)\ge |(Y\setminus X)\cap V_n|.
57
+ \end{equation}
58
+ \item Adding or deleting one element changes every probe by at most
59
+ one. A finite modification with net change $b$ in cardinality satisfies
60
+ $f_n^T(Y)=f_n^T(X)+b$ for all sufficiently large $n$.
61
+ \item Complementation gives
62
+ \[
63
+ f_n^{T^c}(X^c)=-f_n^T(X),\qquad
64
+ \mathcal B^+(T^c)=\{B^c:B\in\mathcal B^-(T)\}.
65
+ \]
66
+ \end{enumerate}
67
+ \end{lemma}
68
+
69
+ \begin{proof}
70
+ The first density limit follows from $X\triangle T\in\mathcal J_0$.
71
+ Also $p_n^T(X)=\sum_{m<n}|W_m|d_m^T(X)$. For any $\varepsilon>0$,
72
+ the terms after a fixed index have absolute density at most
73
+ $\varepsilon$; their contribution divided by $c_n$ is at most
74
+ $\varepsilon$, and the finite initial contribution divided by $c_n$
75
+ tends to zero.
76
+
77
+ Inclusion increases each block count, hence both tail extrema; the
78
+ prefix increases by $|(Y\setminus X)\cap V_n|$. This proves the second
79
+ assertion. If an element changes in a block $W_k$ with $k<n$, only the
80
+ prefix changes. If $k\ge n$, each tail extremum changes by at most
81
+ $1/|W_k|$. By \eqref{eq:block-growth},
82
+ \[
83
+ |W_k|\ge 2\sum_{m<k}|W_m|\ge 2c_n,
84
+ \]
85
+ so the total change is at most one. After every block affected by a
86
+ finite modification is in the prefix, the tails agree and the prefix
87
+ changes by exactly $b$.
88
+
89
+ Finally, complementing both $X$ and $T$ negates every prefix and block
90
+ density. The supremum of the negatives is the negative infimum, and
91
+ vice versa. This proves the last assertion, including its half-open
92
+ endpoint conventions.
93
+ \end{proof}
94
+
95
+ The next continuity statement is needed both to stop finite deletion
96
+ procedures and to pass to their decreasing limit. Its common
97
+ density-zero bound is essential to controlling the tail extrema.
98
+
99
+ \begin{lemma}[Continuity within a fixed interval]\label{lem:block-continuity}
100
+ Suppose $I\subseteq X_k\subseteq Y$ for $k\ge1$, where
101
+ $I,Y\in\mathcal C(T)$, and membership of every element in $X_k$
102
+ eventually agrees with its membership in a set $X$. Then
103
+ $X\in\mathcal C(T)$ and, for every fixed $n\ge1$,
104
+ \[
105
+ f_n^T(X_k)\longrightarrow f_n^T(X).
106
+ \]
107
+ \end{lemma}
108
+
109
+ \begin{proof}
110
+ We have $I\subseteq X\subseteq Y$ and $Y\setminus I\in\mathcal J_0$,
111
+ so $X\in\mathcal C(T)$. On every fixed finite union of blocks, $X_k$
112
+ eventually agrees with $X$. On the remaining blocks,
113
+ \[
114
+ |d_m^T(X_k)-d_m^T(X)|
115
+ \le \frac{|(Y\setminus I)\cap W_m|}{|W_m|},
116
+ \]
117
+ uniformly in $k$, and the right-hand side tends to zero. Thus the
118
+ sequences of block densities converge uniformly in $m$. Supremum and
119
+ infimum over a fixed tail change by at most the uniform difference,
120
+ while the fixed prefix eventually stabilizes. Formula
121
+ \eqref{eq:probes} gives the result.
122
+ \end{proof}
123
+
124
+ \begin{lemma}[Antichains and finite changes]\label{lem:local-antichain}
125
+ Each family $\mathcal B^-(T)$ and $\mathcal B^+(T)$ contains $T$, is
126
+ an antichain under inclusion, and is preserved by finite modifications
127
+ that add and delete equally many elements.
128
+ \end{lemma}
129
+
130
+ \begin{proof}
131
+ The probes of $T$ vanish. Balanced finite changes preserve the class
132
+ and eventually preserve every probe, so they preserve either rule.
133
+
134
+ Suppose $X\subsetneq Y$ both satisfy the lower-limit rule. A finite
135
+ difference of cardinality $k\ge1$ gives
136
+ $\ell_T(Y)=\ell_T(X)+k>0$, a contradiction. For an infinite difference,
137
+ $|(Y\setminus X)\cap V_n|\to\infty$. The probes of $X$ are eventually
138
+ bounded below because their lower limit is finite, so
139
+ Lemma~\ref{lem:probe-properties} implies $f_n^T(Y)\to\infty$, again
140
+ a contradiction. The upper-limit case follows by complementing and
141
+ using the lower-limit rule for $T^c$.
142
+ \end{proof}
143
+
144
+ \subsection{Modifications from a positive pool}
145
+
146
+ To interpolate between subsets, we need to move the limiting probes
147
+ in either direction while remaining in $\mathcal C(T)$. A positive
148
+ pool of available elements suffices, even though we use only a
149
+ density-zero subset of it.
150
+
151
+ \begin{lemma}[Small modifications with divergent probes]\label{lem:positive-pool}
152
+ Let $X\in\mathcal C(T)$.
153
+ If $G\subseteq X^c$ is $\mathcal J_0$-positive, there is
154
+ $P\subseteq G$ in $\mathcal J_0$ such that
155
+ $f_n^T(X\cup P)\to+\infty$.
156
+ If $G\subseteq X$ is $\mathcal J_0$-positive, there is
157
+ $P\subseteq G$ in $\mathcal J_0$ such that
158
+ $f_n^T(X\setminus P)\to-\infty$.
159
+ \end{lemma}
160
+
161
+ \begin{proof}
162
+ For additions, choose $\delta>0$ such that $G$ has density at least
163
+ $\delta$ in arbitrarily late blocks. Suppress the superscript $T$,
164
+ put $a_n=\sup_{m\ge n}|d_m(X)|$, and choose strictly increasing
165
+ positive integers $N_j$ such that, for $n\ge N_j$,
166
+ \begin{equation}\label{eq:spike-cutoff}
167
+ \frac{|p_n(X)|}{c_n}+2a_n+\frac1{\sqrt{c_n}}\le 2^{-j}.
168
+ \end{equation}
169
+ This is possible by Lemma~\ref{lem:probe-properties}.
170
+
171
+ For each sufficiently large $j$, put $b_j=2^{1-j}<\delta$ and choose
172
+ an increasing sequence of blocks $m_j\ge N_{j+1}$ in which $G$ has
173
+ density at least $\delta$, also requiring
174
+ $1/|W_{m_j}|\le\delta-b_j$. From $G\cap W_{m_j}$ select exactly
175
+ $\lceil b_j|W_{m_j}|\rceil$ elements. Rounding is possible because
176
+ this number is at most $\delta|W_{m_j}|$. Let $P$ be the union of these
177
+ selections. Its nonzero block densities lie between $b_j$ and
178
+ $b_j+1/|W_{m_j}|$, and hence tend to zero. Thus $P\in\mathcal J_0$.
179
+
180
+ If $N_j\le n<N_{j+1}$, the selected block $m_j$ belongs to the tail
181
+ in \eqref{eq:probes}. The tail supremum for $X\cup P$ is at least
182
+ $b_j-a_n$, and its tail infimum is at least $-a_n$. The prefix can only
183
+ increase. Therefore \eqref{eq:spike-cutoff} gives
184
+ \[
185
+ \frac{f_n(X\cup P)}{c_n}
186
+ \ge -\frac{|p_n(X)|}{c_n}+b_j-2a_n
187
+ \ge \frac1{\sqrt{c_n}}.
188
+ \]
189
+ These intervals contain every sufficiently large $n$, proving
190
+ divergence to $+\infty$. Apply the addition statement to $X^c$ and
191
+ $T^c$, and use complement symmetry, to obtain the deletion statement.
192
+ \end{proof}
193
+
194
+ \subsection{Interpolation and interval alternatives}
195
+
196
+ The finite-change rule rounds any finite limiting value into the
197
+ interval $(-1,0]$. The remaining case has opposite infinite limits at
198
+ the two endpoints. We handle it by finite deletions whose effect on
199
+ earlier probes is summable.
200
+
201
+ \begin{lemma}[Interpolation]\label{lem:local-interpolation}
202
+ If $I\subseteq Y$ are in $\mathcal C(T)$,
203
+ $\ell_T(I)\le-1$, and $\ell_T(Y)>0$, then there is
204
+ $B\in\mathcal B^-(T)$ with $I\subseteq B\subseteq Y$.
205
+ \end{lemma}
206
+
207
+ \begin{proof}
208
+ Suppress $T$ from the notation. If $\ell(I)=a$ is finite, add
209
+ $\lfloor-a\rfloor$ elements from $Y\setminus I$. There are enough:
210
+ a smaller finite gap of size $h$ would give
211
+ $\ell(Y)=a+h\le-1$. The resulting lower limit belongs to $(-1,0]$.
212
+ If $\ell(Y)=b$ is finite, delete $\lceil b\rceil$ gap elements from
213
+ $Y$. A smaller finite gap of size $h$ would instead give
214
+ $\ell(I)=b-h>0$. Again the resulting lower limit belongs to $(-1,0]$.
215
+
216
+ It remains to consider $\ell(I)=-\infty$ and $\ell(Y)=+\infty$.
217
+ Set $X_0=Y$ and construct decreasing sets $X_j$ by finite deletions.
218
+ At stage $j\ge1$, do nothing if some $n\ge j$ already satisfies
219
+ $f_n(X_{j-1})\le0$. Otherwise choose $M_j\ge j$ so large that
220
+ \begin{equation}\label{eq:stage-loss}
221
+ 2c_j\sup_{m\ge M_j}
222
+ \frac{|(Y\setminus I)\cap W_m|}{|W_m|}<2^{-j}.
223
+ \end{equation}
224
+ This is possible because $Y\setminus I\in\mathcal J_0$.
225
+ Delete elements of $X_{j-1}\setminus I$ in blocks $m\ge M_j$, one
226
+ at a time in increasing block order, stopping as soon as
227
+ $f_n\le0$ for some $n\ge j$.
228
+
229
+ This stopping time is finite. If every eligible element were deleted,
230
+ the resulting set would differ from $I$ by finitely many elements,
231
+ so it would have lower limit $-\infty$. Fix a strictly negative probe
232
+ with index $n\ge j$ for that set. By
233
+ Lemma~\ref{lem:block-continuity}, the same probe is negative after
234
+ finitely many of the deletions. Just before the stopping deletion all
235
+ probes with index at least $j$ were positive. Each drops by at most
236
+ one, so
237
+ \begin{equation}\label{eq:stage-reset}
238
+ f_n(X_j)\ge-1\qquad(n\ge j)
239
+ \end{equation}
240
+ at every stage that makes deletions. For $n<j$ the prefix is unchanged
241
+ during the whole stage, and each tail extremum decreases by at most
242
+ the density supremum in \eqref{eq:stage-loss}. Since $c_n\le c_j$,
243
+ the entire stage decreases $f_n$ by less than $2^{-j}$.
244
+
245
+ Let $X_\infty=\bigcap_{j\ge0}X_j$. It lies between $I$ and $Y$ and
246
+ belongs to $\mathcal C(T)$; Lemma~\ref{lem:block-continuity} applies
247
+ to this decreasing sequence. Every stage leaves a witness
248
+ $f_n\le0$ with $n\ge j$. Such a witness persists under later
249
+ deletions and in the limit, so $\ell(X_\infty)\le0$.
250
+
251
+ There is a first stage $j_0$ that makes deletions. Otherwise the
252
+ unchanged set $Y$ would have a nonpositive probe in every tail,
253
+ contrary to $\ell(Y)=+\infty$. Fix $n\ge j_0$. After stage $j_0$ its
254
+ probe is at least $-1$. Through stage $n$, every later stage either
255
+ leaves it unchanged or restores this bound by \eqref{eq:stage-reset}.
256
+ Stages $j>n$ then cost less than $2^{-j}$ each. Passing to the limit,
257
+ \[
258
+ f_n(X_\infty)\ge-1-\sum_{j>n}2^{-j}=-1-2^{-n}.
259
+ \]
260
+ Consequently $-1\le\ell(X_\infty)\le0$. If the lower limit exceeds
261
+ $-1$, take $B=X_\infty$. If it equals $-1$, add one point of
262
+ $Y\setminus X_\infty$ to obtain lower limit zero. There are infinitely
263
+ many such points: a finite difference from $Y$ would contradict
264
+ $\ell(Y)=+\infty$ by the finite-change rule. This completes the
265
+ interpolation.
266
+ \end{proof}
267
+
268
+ The local rules have the following interval property. Unless a basis
269
+ lies below the lower endpoint, between the endpoints, or above the upper
270
+ endpoint, the prototype has a positive part outside the lower endpoint
271
+ and the upper endpoint has a positive part outside the prototype.
272
+ These are the two differences needed to separate a new prototype class
273
+ from this one in Section~\ref{sec:assembly}.
274
+
275
+ \begin{proposition}[Interval alternatives for one class]
276
+ \label{prop:local-intervals}
277
+ Fix $\sigma\in\{-,+\}$ and let $I\subseteq Y\subseteq E_0$.
278
+ If
279
+ \[
280
+ T\setminus I\in\mathcal J_0
281
+ \quad\text{or}\quad
282
+ Y\setminus T\in\mathcal J_0,
283
+ \]
284
+ there is $B\in\mathcal B^\sigma(T)$ satisfying at least one of
285
+ \begin{equation}\label{eq:local-alternatives}
286
+ B\subseteq I,\qquad I\subseteq B\subseteq Y,
287
+ \qquad Y\subseteq B.
288
+ \end{equation}
289
+ \end{proposition}
290
+
291
+ \begin{proof}
292
+ We first establish the interval alternatives when one or both endpoints
293
+ belong to the class. For the lower-limit rule, if
294
+ $X\in\mathcal C(T)$ has $\ell_T(X)\le-1$,
295
+ Lemmas~\ref{lem:positive-pool} and~\ref{lem:local-interpolation}
296
+ extend it to a basis by additions from any prescribed positive
297
+ subset of $X^c$. If $\ell_T(X)>0$, their deletion versions give a
298
+ basis contained in $X$, using any prescribed positive subset of $X$.
299
+ Both unrestricted corrections are available because $X$ and $X^c$
300
+ are positive.
301
+
302
+ If both $I$ and $Y$ belong to $\mathcal C(T)$, a lower endpoint with
303
+ positive lower limit supplies a basis below $I$, and an upper
304
+ endpoint with lower limit at most $-1$ supplies a basis above $Y$.
305
+ An endpoint that is itself a basis also gives an outcome in
306
+ \eqref{eq:local-alternatives}. The only remaining case is
307
+ $\ell_T(I)\le-1$ and $\ell_T(Y)>0$, when
308
+ Lemma~\ref{lem:local-interpolation} gives a basis between them.
309
+
310
+ If $I$ belongs to the class and $Y\setminus I$ is positive,
311
+ correcting $I$ downwards, leaving it fixed when it is a basis, or
312
+ correcting it upwards from the pool $Y\setminus I$ gives a basis
313
+ below $I$ or between $I$ and $Y$.
314
+ If $Y$ belongs to the class and the gap is positive, the
315
+ corresponding corrections give a basis between $I$ and $Y$ or
316
+ above $Y$.
317
+ Complementation proves these same three conclusions for the
318
+ upper-limit rule, exchanging the two one-endpoint conclusions.
319
+
320
+ Now suppose $T\setminus I\in\mathcal J_0$.
321
+ If $I\in\mathcal C(T)$, a $\mathcal J_0$-small gap puts $Y$ in the same class,
322
+ whereas a positive gap permits the lower-endpoint conclusion just
323
+ proved. In either case we obtain \eqref{eq:local-alternatives}.
324
+ If $I\notin\mathcal C(T)$, then $T\cap I\in\mathcal C(T)$ and
325
+ $I\setminus T$ is positive. Applying the lower-endpoint conclusion
326
+ to $[T\cap I,I]$ gives a basis contained in $I$.
327
+
328
+ Finally, if $Y\setminus T\in\mathcal J_0$, apply the result just
329
+ proved to the prototype $T^c$ and the interval $[Y^c,I^c]$, with
330
+ the opposite rule. Complementing its basis gives
331
+ \eqref{eq:local-alternatives} for $T$ and the original rule.
332
+ \end{proof}
preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/build/sections/05-assembly.tex ADDED
@@ -0,0 +1,342 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Assembling a self-dual matroid}\label{sec:assembly}
2
+
3
+ We now choose the prototype classes to which the local rules will be applied.
4
+ There are two requirements: every resulting basis must impose the desired
5
+ strict inequality on ordinal ranks, and enough classes must be present to
6
+ allow maximal independent extensions inside every subset of $E_0$.
7
+ The interval criterion used for the second requirement is due to
8
+ Bowler and Geschke~\cite[Theorem~6]{BowlerGeschke2016}; we include the full
9
+ verification of the matroid axioms after constructing the bases.
10
+
11
+ \subsection{Admissible sets and two monotone zones}
12
+
13
+ For $X\subseteq E_0=L\dot\cup R$, put
14
+ \[
15
+ u(X)=X_L,\qquad y(X)=D\setminus X_R.
16
+ \]
17
+ Call $X$ \emph{admissible} if either
18
+ \begin{equation}\label{eq:admissible}
19
+ \begin{aligned}
20
+ &u(X),y(X)\in\mathcal U
21
+ &&\text{and }\rho(u(X))>\rho(y(X)),\\
22
+ \text{or }\quad
23
+ &u(X),y(X)\notin\mathcal U
24
+ &&\text{and }\rho(D\setminus u(X))>
25
+ \rho(D\setminus y(X)).
26
+ \end{aligned}
27
+ \end{equation}
28
+ All ranks appearing here are evaluated on members of $\mathcal U$.
29
+ Define the \emph{Upper zone} to consist of those $X$ for which $u(X)$ is
30
+ large and either $y(X)$ is small, or $y(X)$ is large and
31
+ $\rho(u(X))\le\rho(y(X))$.
32
+ Define the \emph{Lower zone} by requiring $X^c$ to lie in the Upper zone.
33
+ Complements of subsets of $E_0$ are taken in $E_0$.
34
+
35
+ \begin{lemma}\label{lem:zones}
36
+ The Upper zone, Lower zone, and admissible sets partition $2^{E_0}$.
37
+ The Upper zone is upward closed, the Lower zone is downward closed,
38
+ and all three statuses are invariant under symmetric differences in
39
+ $\mathcal K_0$.
40
+ Complementation exchanges the two zones and preserves admissibility.
41
+ Moreover, $\varnothing$ is Lower, $E_0$ is Upper, and every admissible
42
+ set and its complement are $\mathcal J_0$-positive.
43
+ \end{lemma}
44
+
45
+ \begin{proof}
46
+ Write $u=u(X)$ and $y=y(X)$.
47
+ When $u$ is large and $y$ small, $X$ is Upper; when $u$ is small and $y$
48
+ large, it is Lower.
49
+ If both are large, comparison of their ranks partitions the possibilities
50
+ into Upper and admissible.
51
+ If both are small, comparison of the ranks of their complements partitions
52
+ the possibilities into Lower and admissible.
53
+ Complementing $X$ replaces both $u$ and $y$ by their complements, proving
54
+ the asserted symmetries.
55
+
56
+ Suppose that $X\subseteq X'$ and $X$ is Upper.
57
+ Then $u\subseteq u'$ and $y'\subseteq y$, with $u'$ large.
58
+ If $y'$ is small, $X'$ is Upper by definition.
59
+ Otherwise $y$ is large as well, and Lemma~\ref{lem:rank} gives
60
+ \[
61
+ \rho(u')\le\rho(u)\le\rho(y)\le\rho(y'),
62
+ \]
63
+ so again $X'$ is Upper.
64
+ Downward closure of the Lower zone follows by complementation.
65
+ The invariance assertion follows from Lemma~\ref{lem:rank} in the two
66
+ coordinates.
67
+ The statuses of $\varnothing$ and $E_0$ follow directly from the definitions.
68
+
69
+ If the first line of~\eqref{eq:admissible} holds, $X_L=u$ and
70
+ $(X^c)_R=y$ are large, hence $\mathcal J$-positive.
71
+ If the second line holds, $X_R=D\setminus y$ and
72
+ $(X^c)_L=D\setminus u$ are large instead.
73
+ In either case $X$ and $X^c$ are $\mathcal J_0$-positive.
74
+ \end{proof}
75
+
76
+ \begin{lemma}[Crossing the zones]\label{lem:zone-crossing}
77
+ If $A\subseteq Z\subseteq E_0$, with $A$ Lower and $Z$ Upper, then
78
+ there is an admissible $B$ satisfying $A\subseteq B\subseteq Z$.
79
+ \end{lemma}
80
+
81
+ \begin{proof}
82
+ The sets $s=A_L$ and $X=Z_L$ are respectively small and large, and
83
+ $s\subseteq X$.
84
+ We keep $B_R=A_R$, so write $y=D\setminus A_R$.
85
+ If $y$ is large, Lemma~\ref{lem:thinning} gives a large $u$ between
86
+ $s$ and $X$ with $\rho(u)>\rho(y)$; take $B_L=u$.
87
+ If $y$ is small, apply the same Lemma between the small set
88
+ $D\setminus X$ and the large set $D\setminus s$ to obtain a large $v$
89
+ with $\rho(v)>\rho(D\setminus y)$.
90
+ Taking $B_L=D\setminus v$ gives the second line
91
+ of~\eqref{eq:admissible}.
92
+ Both constructions respect the two endpoint inclusions.
93
+ \end{proof}
94
+
95
+ \subsection{Reserving separation from earlier classes}
96
+
97
+ Different prototypes must have positive differences in both directions.
98
+ This will ensure that their local bases cannot contain one another.
99
+ The next Lemma arranges these two inequalities while preserving the
100
+ endpoint statuses needed in Lemma~\ref{lem:zone-crossing}.
101
+
102
+ \begin{lemma}\label{lem:insert-prototype}
103
+ Let $\mathcal T$ be a family of fewer than $\mathfrak c$ admissible subsets
104
+ of $E_0$.
105
+ Suppose $A\subseteq Z\subseteq E_0$, that $A$ is not Upper and $Z$ is
106
+ not Lower, and that, for every $T\in\mathcal T$,
107
+ \begin{equation}\label{eq:available-separation}
108
+ T\setminus A\notin\mathcal J_0,
109
+ \qquad Z\setminus T\notin\mathcal J_0.
110
+ \end{equation}
111
+ Then there is an admissible $B$ between $A$ and $Z$ such that
112
+ $B\setminus T$ and $T\setminus B$ are $\mathcal J_0$-positive for every
113
+ $T\in\mathcal T$.
114
+ \end{lemma}
115
+
116
+ \begin{proof}
117
+ Put $G=Z\setminus A$.
118
+ For every $T\in\mathcal T$ with $A\setminus T\in\mathcal J_0$,
119
+ include the trace $G\setminus T$ in a list.
120
+ It is positive by~\eqref{eq:available-separation}, since
121
+ $Z\setminus T=(A\setminus T)\cup(G\setminus T)$.
122
+ For every $T$ with $T\setminus Z\in\mathcal J_0$, also include the
123
+ positive trace $T\cap G$, using
124
+ $T\setminus A=(T\setminus Z)\cup(T\cap G)$.
125
+ There are fewer than $\mathfrak c$ traces.
126
+ Lemma~\ref{lem:reservations} supplies disjoint $\mathcal K_0$-small sets
127
+ $H_0,H_1$ that meet every listed trace $\mathcal J_0$-positively.
128
+ An empty list presents no restriction on their choice.
129
+
130
+ Modify only the gap:
131
+ \begin{equation}\label{eq:gap-reservations}
132
+ A'=A\cup(H_0\cap G),\qquad
133
+ Z'=Z\setminus(H_1\cap G).
134
+ \end{equation}
135
+ Because $H_0$ and $H_1$ are disjoint and $G$ is disjoint from $A$, we have
136
+ $A'\subseteq Z'$.
137
+ The endpoint changes are $\mathcal K_0$-small, so $A'$ is not Upper and
138
+ $Z'$ is not Lower by Lemma~\ref{lem:zones}.
139
+ If an endpoint is admissible, take it for $B$.
140
+ Otherwise $A'$ is Lower and $Z'$ Upper, and
141
+ Lemma~\ref{lem:zone-crossing} gives an admissible $B$ between them.
142
+
143
+ For any $T\in\mathcal T$, if $A\setminus T$ is positive then so is
144
+ $B\setminus T$.
145
+ Otherwise the reserved positive set $H_0\cap(G\setminus T)$ lies in
146
+ $B\setminus T$.
147
+ Likewise, if $T\setminus Z$ is positive it is already contained in
148
+ $T\setminus B$; otherwise the reserved positive set $H_1\cap T\cap G$
149
+ is contained in $T\setminus B$.
150
+ This proves both inequalities.
151
+ \end{proof}
152
+
153
+ \subsection{Meeting every interval}
154
+
155
+ We choose admissible prototypes in complementary pairs.
156
+ For each first prototype $T$ we retain the local bases
157
+ $\mathcal B^-(T)$, and for $T^c$ we retain $\mathcal B^+(T^c)$.
158
+ These two families are complements of one another by the local rules.
159
+ Once a pair has been inserted, its rule and all its bases remain fixed.
160
+ The aim is that, for every interval $I\subseteq Y\subseteq E_0$ with infinite gap,
161
+ some basis $B$ satisfies the following alternative:
162
+ \begin{equation}\label{eq:interval-alternative}
163
+ B\subseteq I,\qquad I\subseteq B\subseteq Y,
164
+ \qquad\text{or}\qquad Y\subseteq B.
165
+ \end{equation}
166
+
167
+ \begin{proposition}\label{prop:basis-family}
168
+ There is a nonempty family $\mathcal B$ of admissible subsets of $E_0$
169
+ with the following properties:
170
+ \begin{enumerate}
171
+ \item $\mathcal B$ is an antichain and is closed under complements.
172
+ \item If $B\in\mathcal B$, $F\subseteq B$ and $H\subseteq E_0\setminus B$
173
+ are finite with $|F|=|H|$, then $(B\setminus F)\cup H\in\mathcal B$.
174
+ \item For every $I\subseteq Y\subseteq E_0$ with $Y\setminus I$ infinite,
175
+ the alternative~\eqref{eq:interval-alternative} holds.
176
+ \end{enumerate}
177
+ \end{proposition}
178
+
179
+ \begin{proof}
180
+ As $E_0$ is countable, list all intervals with infinite gap in a sequence
181
+ of length $\mathfrak c$.
182
+ Recursively retain complementary pairs of admissible prototypes, requiring
183
+ the two directed differences of any distinct prototypes to be
184
+ $\mathcal J_0$-positive.
185
+ At any stage, call bases in the already retained local families
186
+ \emph{old bases}.
187
+ They are closed under complements.
188
+
189
+ Consider the current interval $I\subseteq Y$.
190
+ If~\eqref{eq:interval-alternative} already holds for an old basis,
191
+ skip this stage. Otherwise Proposition~\ref{prop:local-intervals}
192
+ implies that every old prototype $T$ satisfies
193
+ \begin{equation}\label{eq:unmet-interval}
194
+ T\setminus I\notin\mathcal J_0,
195
+ \qquad Y\setminus T\notin\mathcal J_0.
196
+ \end{equation}
197
+ Thus an unmet interval has the positive differences needed to reserve
198
+ separation from every old class.
199
+
200
+ An admissible set cannot contain an Upper set or be contained in a Lower
201
+ set, by Lemma~\ref{lem:zones}. Thus if $I$ is Upper, we must seek the
202
+ allowed basis below $I$; if $Y$ is Lower, we must seek it above $Y$.
203
+ Otherwise we seek a basis between the endpoints. Accordingly choose
204
+ \[
205
+ [A,Z]=
206
+ \begin{cases}
207
+ [\varnothing,I],& I\text{ is Upper},\\
208
+ [Y,E_0],&Y\text{ is Lower},\\
209
+ [I,Y],&\text{otherwise}.
210
+ \end{cases}
211
+ \]
212
+ The first two cases cannot coincide, by monotonicity of the Upper zone.
213
+ In every case $A$ is not Upper and $Z$ is not Lower.
214
+ We verify~\eqref{eq:available-separation} for all old prototypes.
215
+ In the third case it is~\eqref{eq:unmet-interval}.
216
+ In the first case $T\setminus A=T$ is positive.
217
+ If $I\setminus T$ were $\mathcal J_0$-small, $I\cap T$ would remain Upper and be
218
+ contained in $T$, forcing the admissible $T$ to be Upper.
219
+ Thus $Z\setminus T=I\setminus T$ is positive.
220
+ In the second case $Z\setminus T=T^c$ is positive.
221
+ If $T\setminus Y$ were $\mathcal J_0$-small, $T\cap Y$ would remain admissible and be
222
+ contained in the Lower set $Y$, a contradiction.
223
+ Thus $T\setminus A=T\setminus Y$ is positive as well.
224
+
225
+ At a stage $\alpha<\mathfrak c$ there are at most two prototypes per
226
+ earlier stage, hence fewer than $\mathfrak c$ old prototypes.
227
+ Lemma~\ref{lem:insert-prototype} therefore supplies an admissible $B$
228
+ between $A$ and $Z$ with both positive differences from every old
229
+ prototype.
230
+ Insert $B$ with the minus rule and $B^c$ with the plus rule.
231
+ The complement has both positive differences from every old $T$, because
232
+ $T^c$ is also old and
233
+ \[
234
+ B^c\setminus T=T^c\setminus B,\qquad
235
+ T\setminus B^c=B\setminus T^c.
236
+ \]
237
+ The two new prototypes have positive differences from one another by
238
+ Lemma~\ref{lem:zones}.
239
+ They therefore define new classes.
240
+ All probes of $B$ relative to itself vanish, so $B\in\mathcal B^-(B)$.
241
+ Its placement in $[A,Z]$ supplies one of the three outcomes
242
+ in~\eqref{eq:interval-alternative} for the original interval.
243
+
244
+ This recursion uses no regularity assumption on $\mathfrak c$.
245
+ For each individual $\alpha$ below its initial ordinal, the numbers of
246
+ predecessors, prototypes, and requested traces are all bounded by a fixed
247
+ cardinal less than $\mathfrak c$.
248
+ The reservation Lemma applies with that bound.
249
+ Choices can be made using a fixed well-order of $2^{E_0}$.
250
+
251
+ Let $\mathcal B$ be the union of all retained local basis families.
252
+ It is nonempty, since the interval $[\varnothing,E_0]$ receives an outcome.
253
+ Every member remains admissible under its $\mathcal J_0$-small change
254
+ from its prototype, and the family is closed under complements.
255
+ Lemma~\ref{lem:local-antichain} gives the antichain and finite-change
256
+ properties within each class.
257
+ For different classes, the positive directed differences of their
258
+ prototypes remain positive after $\mathcal J_0$-small changes.
259
+ Thus their bases are incomparable as well.
260
+ Finally every interval outcome persists, because no local family is
261
+ subsequently altered.
262
+ \end{proof}
263
+
264
+ \subsection{The maximal-extension axiom}
265
+
266
+ The interval construction is complete.
267
+ We now check that it produces a matroid, including maximal extension
268
+ inside arbitrary subsets; finite exchange alone does not supply this
269
+ last property.
270
+
271
+ \begin{theorem}\label{thm:local-matroid}
272
+ There is a matroid $Q$ on $E_0=L\dot\cup R$ whose bases are precisely
273
+ the family $\mathcal B$ in Proposition~\ref{prop:basis-family}.
274
+ It is equal to its dual on the same labels, and all its bases are admissible.
275
+ In particular, for every basis $B$,
276
+ \begin{equation}\label{eq:basis-rank-decrease}
277
+ B_L\in\mathcal U
278
+ \quad\Longrightarrow\quad
279
+ D\setminus B_R\in\mathcal U
280
+ \quad\text{and}\quad
281
+ \rho(B_L)>\rho(D\setminus B_R).
282
+ \end{equation}
283
+ Every independent set of $Q$ that is not a basis can be extended by any
284
+ element outside it.
285
+ \end{theorem}
286
+
287
+ \begin{proof}
288
+ Define the independent sets to be all subsets of members of $\mathcal B$.
289
+ Since $\mathcal B$ is nonempty, this gives (I1), and heredity (I2) is
290
+ immediate.
291
+ The maximal independent sets are exactly $\mathcal B$:
292
+ each independent set is contained in a member, and the antichain property
293
+ prevents any such member from having a proper independent extension.
294
+
295
+ Suppose $I$ is independent but not maximal, and choose $B_0\in\mathcal B$
296
+ properly containing it.
297
+ Let $e\in E_0\setminus I$.
298
+ If $e\in B_0$, then $I\cup\{e\}$ is independent.
299
+ Otherwise choose $f\in B_0\setminus I$; the balanced swap
300
+ $(B_0\setminus\{f\})\cup\{e\}$ is a basis containing $I\cup\{e\}$.
301
+ This proves the final assertion of the theorem.
302
+ For any maximal independent $B_1$, its difference $B_1\setminus I$ is
303
+ nonempty, since $B_1\subseteq I$ would contradict its maximality.
304
+ Taking $e$ from this difference proves (I3).
305
+
306
+ For (IM), fix an independent $I\subseteq Y\subseteq E_0$.
307
+ If $Y\setminus I$ is finite, choose an independent extension of $I$
308
+ containing a maximum number of elements of that finite gap.
309
+ It is maximal within $Y$.
310
+ If the gap is infinite, use~\eqref{eq:interval-alternative}.
311
+ A basis $B\subseteq I$ forces $B=I$: put $I$ inside a basis $B'$ and
312
+ apply the antichain property to $B\subseteq I\subseteq B'$.
313
+ Thus in this case $I$ itself is maximal within $Y$.
314
+ A basis between $I$ and $Y$ is the required maximal extension.
315
+ A basis containing $Y$ makes $Y$ independent, so $Y$ itself is the
316
+ required extension.
317
+ This proves all four independent-set axioms.
318
+
319
+ The bases of the dual matroid are the complements of the bases of $Q$.
320
+ Since $\mathcal B$ is complement-closed, $Q^*=Q$ on $E_0$.
321
+ Admissibility was established in Proposition~\ref{prop:basis-family},
322
+ and~\eqref{eq:basis-rank-decrease} is its first case.
323
+ \end{proof}
324
+
325
+ \begin{remark}\label{rem:uniform-local}
326
+ The matroid $Q$ is uniform in the sense that every subset is independent
327
+ or spanning~\cite{BowlerGeschke2016}.
328
+ Indeed, if $X$ is dependent, maximize an independent subset $I$ inside
329
+ $X$ using (IM).
330
+ If $I$ were not a basis of $Q$, the last assertion of
331
+ Theorem~\ref{thm:local-matroid} would allow another element of $X$ to be
332
+ added.
333
+ Thus $X$ contains a basis and is spanning.
334
+ Every basis and its complement are infinite by admissibility, so $Q$
335
+ has infinite rank and corank.
336
+ Every finite $F\subseteq E_0$ is independent: starting from any basis,
337
+ insert the elements of $F$ that are missing and delete equally many
338
+ elements outside $F$, using its infinitude and balanced finite changes.
339
+ Yet $E_0$ is dependent, because every basis has a nonempty complement.
340
+ Thus $Q$ is not finitary, and self-duality shows that it is not cofinitary
341
+ either.
342
+ \end{remark}
preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/build/sections/06-counterexample.tex ADDED
@@ -0,0 +1,153 @@
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
1
+ \section{Two matroids on a double ray}\label{sec:counterexample}
2
+
3
+ We now use the local matroid $Q$ from
4
+ Theorem~\ref{thm:local-matroid} to construct the required pair.
5
+ Recall that $Q=Q^*$ on $E_0=L\mathbin{\dot\cup}R$, where each
6
+ of $L,R$ is a labeled copy of the countable set $D$. The ultrafilter
7
+ $\mathcal U$ and ordinal rank $\rho$ have the following consequence
8
+ for every basis $B$ of $Q$:
9
+ \begin{equation}\label{eq:outward-rank}
10
+ B_L\in\mathcal U
11
+ \quad\Longrightarrow\quad
12
+ D\setminus B_R\in\mathcal U
13
+ \quad\text{and}\quad
14
+ \rho(B_L)>\rho(D\setminus B_R).
15
+ \end{equation}
16
+ The rank is antitone under inclusion of members of $\mathcal U$.
17
+ An independent covering will propagate a member of $\mathcal U$
18
+ along a ray, strictly decreasing this rank at every step.
19
+
20
+ \subsection{Direct sums and the common ground set}
21
+
22
+ For completeness, the direct sums we use satisfy all the infinite-matroid
23
+ axioms. Let $(Q_j:j\in J)$ be matroids on pairwise disjoint sets $F_j$,
24
+ where $J$ is countable. Declare $I\subseteq\bigcup_{j\in J}F_j$
25
+ independent if $I\cap F_j$ is independent in every $Q_j$.
26
+ Axioms (I1) and (I2) follow componentwise. The maximal independent
27
+ sets are exactly the unions of one basis from each component: a
28
+ nonmaximal component permits an extension of the union, and if all
29
+ components are maximal no element can be adjoined.
30
+
31
+ For (I3), if $I$ is not maximal, some $I\cap F_j$ is not maximal
32
+ in $Q_j$. Given a global basis $B$, its part $B\cap F_j$ is a
33
+ component basis. Apply (I3) there and adjoin the resulting element to
34
+ $I$. For (IM), given independent $I\subseteq Y$, choose in each
35
+ component a maximal independent extension of $I\cap F_j$ inside
36
+ $Y\cap F_j$. Their union is a maximal independent extension of $I$
37
+ inside $Y$. These choices are available in ZFC. This proves that the
38
+ direct sum is a matroid, and also proves its stated description of
39
+ bases. If every component is self-dual on its own labels, then the
40
+ complement of each global basis is again a global basis, so the direct
41
+ sum is self-dual on the same labels.
42
+
43
+ Take vertices $v_n$ indexed by $n\in\mathbb Z$. Between $v_n$ and
44
+ $v_{n+1}$ put the bundle
45
+ \[
46
+ e_n=\{n\}\times D,
47
+ \qquad E=\mathop{\dot\bigcup}_{n\in\mathbb Z}e_n.
48
+ \]
49
+ Thus every bundle has the fixed label map $(n,d)\mapsto d$ onto $D$.
50
+ The ground set $E$ is countably infinite: $D$ is a countably infinite
51
+ union of nonempty finite blocks, and $E=\mathbb Z\times D$.
52
+ Designate $e_{-1}$, joining $v_{-1}$ and $v_0$, as the central bundle.
53
+ At every vertex put a copy $Q_n$ of $Q$ on $e_{n-1}\cup e_n$.
54
+ The inward bundle is its $L$-coordinate, and the outward bundle its
55
+ $R$-coordinate; explicitly,
56
+ \[
57
+ \begin{array}{c|cc}
58
+ &L&R\\\hline
59
+ n\le -1&e_n&e_{n-1}\\
60
+ n\ge 0&e_{n-1}&e_n.
61
+ \end{array}
62
+ \]
63
+ Both middle vertices therefore use the central bundle as $L$.
64
+ All copies use the same label maps, ultrafilter, and rank.
65
+
66
+
67
+
68
+ Define
69
+ \[
70
+ M_0=\bigoplus_{n\in 2\mathbb Z}Q_n,
71
+ \qquad
72
+ M_1=\bigoplus_{n\in 2\mathbb Z+1}Q_n.
73
+ \]
74
+ For either parity, the component supports partition $E$, since each
75
+ bundle has exactly one endpoint of that parity. Hence these are
76
+ matroids on the same countably infinite set $E$. The preceding
77
+ direct-sum verification and $Q=Q^*$ give $M_i=M_i^*$ on the same
78
+ labels for $i=0,1$.
79
+
80
+ The parity placement and inward/outward coordinates are shown in
81
+ Figure~\ref{fig:double-ray}.
82
+
83
+ \begin{figure}[htbp]
84
+ \centering
85
+ \input{figures/double-ray.tex}
86
+ \caption{Each segment represents a copy of $D$. A copy of $Q$ uses
87
+ the two bundles incident with its vertex. Filled vertices contribute
88
+ to $M_0$, open vertices to $M_1$. The central bundle is $e_{-1}$;
89
+ from either endpoint, the $L$-coordinate points toward the center and
90
+ the $R$-coordinate points outward.}
91
+ \label{fig:double-ray}
92
+ \end{figure}
93
+
94
+ Every finite subset of $E$ is independent in each $M_i$, because
95
+ all its component parts are finite and every finite subset of $Q$ is
96
+ independent by Remark~\ref{rem:uniform-local}. But $E$ is dependent
97
+ in each $M_i$: its intersection with any component support is the
98
+ dependent whole ground set of that copy of $Q$. Thus neither $M_i$
99
+ is finitary. Since $M_i=M_i^*$, neither is cofinitary either.
100
+
101
+ In fact, neither matroid has a nonempty finitary or cofinitary direct
102
+ summand. Suppose a nonempty set $F$ supports a finitary summand.
103
+ Every subset of $F$ is independent, since all its finite subsets are
104
+ independent, so $F$ is the summand's only basis. Thus every basis of
105
+ $M_i$ contains $F$. But complements of bases are also bases of $M_i$,
106
+ a contradiction. Dualizing the direct-sum basis description gives the
107
+ same contradiction for a cofinitary summand.
108
+
109
+ \subsection{The descending ranks}
110
+
111
+ Suppose that independent sets $J_i$ of $M_i$ cover $E$.
112
+ Replacing $J_1$ by $E\setminus J_0\subseteq J_1$, we obtain an
113
+ independent partition $E=J_0\mathbin{\dot\cup}J_1$.
114
+ Assign each element of a bundle to the endpoint whose parity agrees
115
+ with its part in this partition. At every vertex, the assigned elements
116
+ on its two incident bundles form an independent set of its copy of $Q$.
117
+
118
+ The central bundle is partitioned between $v_{-1}$ and $v_0$.
119
+ Exactly one of the two label sets belongs to $\mathcal U$.
120
+ Start at that endpoint and move outward forever. Write $x_k\subseteq D$
121
+ for the labels received by the $k$th vertex on its inward bundle.
122
+ Thus $x_0\in\mathcal U$. If the current vertex receives $z_k$
123
+ on its outward bundle, the next vertex receives exactly
124
+ \[
125
+ x_{k+1}=D\setminus z_k
126
+ \]
127
+ there, because the assignment is a partition and the label maps agree.
128
+
129
+ Assume inductively that $x_k\in\mathcal U$. The independent
130
+ assignment at this vertex is contained in a basis $B_k$ of its copy
131
+ of $Q$. Put
132
+ \[
133
+ u_k=(B_k)_L,
134
+ \qquad y_k=D\setminus(B_k)_R.
135
+ \]
136
+ We have $x_k\subseteq u_k$, so $u_k\in\mathcal U$.
137
+ Equation~\eqref{eq:outward-rank} gives $y_k\in\mathcal U$ and
138
+ $\rho(u_k)>\rho(y_k)$. Since $z_k\subseteq(B_k)_R$,
139
+ we have $y_k\subseteq x_{k+1}$; hence $x_{k+1}\in\mathcal U$.
140
+ Antitonicity now yields
141
+ \begin{equation}\label{eq:ordinal-descent}
142
+ \rho(x_k)\ \ge\ \rho(u_k)\ >\ \rho(y_k)\ \ge\
143
+ \rho(x_{k+1}).
144
+ \end{equation}
145
+ This produces an infinite strictly descending sequence of ordinals,
146
+ which is impossible: its set of values has a least element, and the
147
+ next value would be smaller.
148
+
149
+ Thus $M_0,M_1$ have no independent covering of $E$.
150
+ By Lemma~\ref{lem:selfdual-reduction}, they have no packing/covering
151
+ partition either. Their common ground set is countably infinite and
152
+ both matroids are self-dual on the same labels, completing the proof
153
+ of Theorem~\ref{thm:main}.
preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/build/sections/07-consequences.tex ADDED
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+ \section{The separate Covering and Packing conjectures}
2
+ \label{sec:separate-consequences}
3
+
4
+ Bowler and Carmesin also formulated separate Covering and Packing
5
+ conjectures. For a set-indexed family $\mathcal M=(M_i:i\in\Theta)$ on $E$,
6
+ write $\mathcal M\!\upharpoonright Y=(M_i\!\upharpoonright Y:i\in\Theta)$
7
+ and $\mathcal M.Y=(M_i.Y:i\in\Theta)$. Their Covering Conjecture asserts,
8
+ for every such family, the equivalence
9
+ \begin{equation}\label{eq:covering-conjecture}
10
+ \begin{aligned}
11
+ &\mathcal M\text{ has a covering}\\
12
+ &\quad\Longleftrightarrow\quad
13
+ \text{for every }Y\subseteq E,\\
14
+ &\qquad\bigl[\mathcal M\!\upharpoonright Y\text{ has a packing}
15
+ \Longrightarrow
16
+ \mathcal M\!\upharpoonright Y\text{ has a covering}\bigr].
17
+ \end{aligned}
18
+ \end{equation}
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+ Their Packing Conjecture asserts, again for every such family,
20
+ \begin{equation}\label{eq:packing-conjecture}
21
+ \begin{aligned}
22
+ &\mathcal M\text{ has a packing}\\
23
+ &\quad\Longleftrightarrow\quad
24
+ \text{for every }Y\subseteq E,\\
25
+ &\qquad\bigl[\mathcal M.Y\text{ has a covering}
26
+ \Longrightarrow
27
+ \mathcal M.Y\text{ has a packing}\bigr].
28
+ \end{aligned}
29
+ \end{equation}
30
+ These are the conjectures of~\cite[Conjectures~5.2 and~6.3]{BowlerCarmesin2015}.
31
+
32
+ \begin{corollary}\label{cor:separate-covering-packing}
33
+ The unrestricted separate Covering and Packing Conjectures of Bowler and
34
+ Carmesin are both false in ZFC.
35
+ \end{corollary}
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+
37
+ \begin{proof}
38
+ Bowler and Carmesin's universal equivalences identify intersection for
39
+ every pair, packing/covering for every pair, packing/covering for every
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+ set-indexed family, \eqref{eq:covering-conjecture} for every set-indexed
41
+ family, and \eqref{eq:packing-conjecture} for every set-indexed family
42
+ \cite[Section~7]{BowlerCarmesin2015}. Theorem~\ref{thm:main} falsifies the
43
+ pairwise packing/covering assertion, so both separate universal conjectures
44
+ are false. These last two failures are consequences of equivalence between
45
+ universal statements; this argument does not identify their witnessing
46
+ families with the pair $(M_0,M_1)$.
47
+ \end{proof}
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+
preprints/A-Counterexample-to-the-Infinite-Matroid-Packing-Covering-Conjecture-September-24-2026/paper.pdf ADDED
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