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3b2b6f3ca477f403dc0947fee08906f9633835f5
subsection
32
34
Example derivations
Here is the derivation of this equation:((x \mathop {{}_{1}\!{?}\!_{1}} y) \mathop {?_{p}} x) \mathop {?_{p}} (y \mathop {?_{p}} (x \mathop {{}_{1}\!{?}\!_{1}} y)) & = ((x \mathop {{}_{1}\!{?}\!_{1}} y) \mathop {?_{p}} (x \mathop {{}_{1}\!{?}\!_{1}} x)) \mathop {?_{p}} ((y \mathop {{}_{1}\!{?}\!_{1}} y) \mathop {?_{p}}...
{ "cite_spans": [] }
10.4230/LIPIcs.ICALP.2018.141
1802.09598
The Beta-Bernoulli process and algebraic effects
[ "Sam Staton", "Dario Stein", "Hongseok Yang", "Nathanael L. Ackerman", "Cameron E. Freer", "Daniel M. Roy" ]
[ "cs.PL" ]
2,018
en
Computer Science
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d4f03e3155ed8a615b13b696b7ffdd318a3f80e0
subsection
33
34
Example derivations
Making (t \mathop {?_{p}} x) \mathop {?_{p}} (y \mathop {?_{p}} t) permutation-invariant means computing the average(t \mathop {?_{p}} x) \mathop {?_{p}} (y \mathop {?_{p}} t)&= ((t \mathop {?_{p}} x) \mathop {?_{p}} (y \mathop {?_{p}} t)) \mathop {{}_{1}\!{?}\!_{1}} ((t \mathop {?_{p}} y) \mathop {?_{p}} (x \mathop {?...
{ "cite_spans": [] }
10.4230/LIPIcs.ICALP.2018.141
1802.09598
The Beta-Bernoulli process and algebraic effects
[ "Sam Staton", "Dario Stein", "Hongseok Yang", "Nathanael L. Ackerman", "Cameron E. Freer", "Daniel M. Roy" ]
[ "cs.PL" ]
2,018
en
Computer Science
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730321149c8cd56a1f5ae352161b30f0c600235f
abstract
0
1,121
Abstract
This book introduces a new context for global homotopy theory, i.e., equivariant homotopy theory with universal symmetries. Many important equivariant theories naturally exist not just for a particular group, but in a uniform way for all groups in a specific class. Prominent examples are equivariant stable homotopy, eq...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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dcc5ae2873cc384ba460e7b5f9f7df986b440493
subsection
1
1,121
Preface
Equivariant stable homotopy theory has a long tradition, starting from geometrically motivated questions about symmetries of manifolds. The homotopy theoretic foundations of the subject were laid by tom Dieck, Segal and May and their students and collaborators in the 70's, and during the last decades equivariant stable...
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10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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1fc9d75d5c16e9d273efff287115c7d4af88f855
subsection
2
1,121
Preface
By Theorem REF this forgetful functor has a left adjoint L and a right adjoint R, both fully faithful, that participate in a recollement of triangulated categories:@C=15mm{ {\mathcal {GH}}^+ @<-.3ex>[r]^-{i_*} & {\mathcal {GH}}\ @<-.3ex>[r]^-U \ @<.4ex>@/^1pc/[l]^-{i^!} @<-.4ex>@/_1pc/[l]_-{i^*} & {\mathcal {SH}}\ @<.4...
{ "cite_spans": [ { "arxiv_id": "", "doi": "", "end": 1988, "openalex_id": "", "raw": "F. Morel, V. Voevodsky, {\\mathbb {A}}^1-homotopy theory of schemes. Inst. Hautes Études Sci. Publ. Math. 90 (1999), 45–143.", "source_ref_id": "72023045a955860bc6365604ec4aeaf285b7472c", ...
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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7c1202906ee00a67539876390e34ba8d0528f92e
subsection
3
1,121
Preface
We discuss these different global forms of B O is some detail in Section , and the associated Thom spectra in Section .In the stable global world, every non-equivariant homotopy type has two extreme global refinements, the `left induced' (the global analog of a constant orthogonal space, see Example REF ) and the `righ...
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10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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3eac0e58dc498e6de631cb93b5b3197aa7960042
subsection
4
1,121
Preface
The class of trivial groups is also admissible here, but then we just recover the `traditional' stable category. If the family {\mathcal {F}} is multiplicative, then the {\mathcal {F}}-global model structure is monoidal with respect to the smash product of orthogonal spectra and satisfies the monoid axiom (Proposition ...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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f5706f4523561633433e2a1312f71110388b406e
subsection
5
1,121
Preface
However, since the group G is not intrinsic and can vary, one needs equivariant cohomology theories for all groups G, with some compatibility.Part of the compatibility can be deduced from the fact that the same orbifold can be presented in different ways; for example, if G is a closed subgroup of K, then the global quo...
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10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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86cdbf3601e3960b4e17a0e99ecc328c1fe83f81
subsection
6
1,121
Preface
By the adjunction relating the global and G-equivariant stable homotopy categories (see Theorem REF ), the morphisms \llbracket \Sigma ^\infty _+ {\mathbf {L}}_{G,V}M, E\rrbracket in the global stable homotopy category biject with the G-equivariant E-cohomology groups of M. In other words, when evaluated on a global qu...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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7ad17905db9844045d36520b1b47e401aad9c2d6
subsection
7
1,121
Preface
The study of natural operations on \pi _0^G(Y) is a recurring theme throughout this book; in the later chapters we return to it in the contexts of ultra-commutative monoids, orthogonal spectra and ultra-commutative ring spectra.Chapter is devoted to ultra-commutative monoids (a.k.a. commutative monoids with respect to ...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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909e0695e299837664322d07448d422c31586109
subsection
8
1,121
Preface
Here we work more generally relative to a global family {\mathcal {F}} and consider the {\mathcal {F}}-equivalences (i.e., equivariant stable equivalences for all compact Lie groups in the family {\mathcal {F}}). We follow the familiar outline: a certain {\mathcal {F}}-level model structure is Bousfield localized to an...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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e4d143ea1151d49b0f945ebc2d1518c8e375a5f2
subsection
9
1,121
Preface
The equivariant homology theory represented by {\mathbf {MO}} can be obtained from the one represented by {\mathbf {mO}} in an algebraic fashion, by inverting the collection of `inverse Thom classes', compare Corollary REF . Section recalls the geometrically defined equivariant bordism theories. The Thom-Pontryagin con...
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10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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5f84fba65dd36581252c2ce1cc1670da608856f9
subsection
10
1,121
Preface
However, we do prove in Theorem REF that evaluating a G-cofibrant special {\mathbf {\Gamma }}-G-space on spheres yields a `G^\circ -trivial positive G-\Omega -spectrum', where G^\circ is the identity component of G. Our Appendix REF substantially overlaps with the paper by May, Merling and Osorno that provides compari...
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10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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486a6e4572a2bb4d8a80a014516ad527e51827ce
subsection
11
1,121
Preface
In particular, by simply ignoring all group actions, the examples presented in this book give models for many interesting and prominent non-equivariant stable homotopy types.Since actions of compact Lie groups are central to this book, some familiarity with the structure and representation theory of compact Lie groups ...
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10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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3e9290aa1f5f311836ba4121a50ce2a82af3595f
subsection
12
1,121
Unstable global homotopy theory
In this chapter we develop a framework for unstable global homotopy theory via orthogonal spaces, i.e., continuous functors from the linear isometries category {\mathbf {L}} to spaces. In Section we define global equivalences of orthogonal spaces and establish many basic properties of this class of morphisms. We also i...
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10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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fc59378ba2ab62a8525afae3b66aa2a7d6ac06ef
subsection
13
1,121
Orthogonal spaces and global equivalences
In this section we introduce orthogonal spaces, along with the notion of global equivalences, our setup to rigorously formulate the idea of `compatible equivariant homotopy types for all compact Lie groups'. We introduce various basic techniques to manipulate global equivalences of orthogonal spaces, such as recognitio...
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10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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9040898e3384beaaf2fa185842ae45a40f0e7f69
subsection
14
1,121
Orthogonal spaces and global equivalences
So the full topological subcategory with objects the {\mathbb {R}}^n is a small skeleton of {\mathbf {L}}.Definition 1.1 An orthogonal spaceorthogonal space is a continuous functor Y:{\mathbf {L}}\longrightarrow {\mathbf {T}} to the category of spaces. A morphism of orthogonal spaces is a natural transformation. We de...
{ "cite_spans": [ { "arxiv_id": "", "doi": "", "end": 692, "openalex_id": "", "raw": "J. M. Boardman, On Stable Homotopy Theory and Some Applications. PhD thesis, University of Cambridge (1964).", "source_ref_id": "c7b9425c4068b352d831b65a97be79245f5fcad3", "start": 543 ...
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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7204c9ba5a1711695c19f4198bb250ba7462a6f6
subsection
15
1,121
Orthogonal spaces and global equivalences
In particular, D^0=\lbrace 0\rbrace is a one-point space and \partial D^0=\emptyset is empty.Definition 1.2 A morphism f:X\longrightarrow Y of orthogonal spaces is a global equivalenceglobal equivalence!of orthogonal spaces if the following condition holds: for every compact Lie group G, every G-representation V, eve...
{ "cite_spans": [ { "arxiv_id": "", "doi": "", "end": 2132, "openalex_id": "https://openalex.org/W2129539457", "raw": "J. P. May, A concise course in algebraic topology. Chicago Lectures in Mathematics. University of Chicago Press, Chicago, IL, 1999. x+243 pp.", "source_ref_id"...
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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f6e7e8aac8cdc734bfb625fa797017238b739a76
subsection
16
1,121
Orthogonal spaces and global equivalences
So \underline{g} is a global equivalence if and only if g is a weak equivalence.Remark 1.4 The notion of global equivalence is meant to capture the idea that for every compact Lie group G, some induced morphism\operatorname{hocolim}_V f(V)\ :\ \operatorname{hocolim}_V X(V)\ \longrightarrow \ \operatorname{hocolim}_V Y(...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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8085535cfd206b2c50a6eda485ddbb7ee98884c9
subsection
17
1,121
Orthogonal spaces and global equivalences
We suppose that the lifting problem (H_0,K_0) has a solution consisting of a continuous map \lambda :B\longrightarrow X such that \lambda |_A=H_0 and a homotopy G:B\times [0,1]\longrightarrow Y such thatG_0 \ = \ f\circ \lambda \ , \quad G_1\ = \ K_0 \text{\qquad and\qquad } (G_t)|_A \ = \ f\circ H_0for all t\in [0,1]....
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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0111843a6c846809ce3cfe682c220db2757c9757
subsection
18
1,121
Orthogonal spaces and global equivalences
We define a continuous map L:A\times [0,3]\times [0,1]\longrightarrow Y byL(-,t,s) \ = \ {\left\lbrace \begin{array}{ll} f\circ H_{1-t} & \text{ for $0\le t\le s$, }\\ f\circ H_{1-s} & \text{ for $s\le t\le 3-s$, and}\\ f\circ H_{t-2} & \text{ for $3-s\le t\le 3$.} \end{array}\right.}Then L(-,-,0) is the constant homot...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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731a35e559475715dd0870c17ec39b5f7ac72284
subsection
19
1,121
Orthogonal spaces and global equivalences
The map \bar{J}=\bar{L}(-,-,0):B\times [0,3]\longrightarrow Y then satisfies\bar{J}|_{A\times [0,3]}\ = \ \bar{L}(-,-,0)|_{A\times [0,3]}\ = \ L(-,-,0)\ ,which is the constant homotopy at the map f\circ H_1; so \bar{J} is a homotopy (parametrized by [0,3] instead of [0,1]) relative to A. Because\bar{J}_0 \ = \ \bar{L}(...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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4efbc266fadd7172e6f841680da633cefe016c8c
subsection
20
1,121
Orthogonal spaces and global equivalences
For every compact Lie group G and every exhaustive sequence \lbrace V_i\rbrace _{i\ge 1} of G-representations the induced map \operatorname{tel}_i f(V_i)\ : \ \operatorname{tel}_i X(V_i)\ \longrightarrow \ \operatorname{tel}_i Y(V_i) is a G-weak equivalence.At various places in the proof we use without explicit menti...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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1ee228407990ed2cee450dfb222ed08d243e66a4
subsection
21
1,121
Orthogonal spaces and global equivalences
Since f is a global equivalence, there is an H-equivariant linear isometric embedding \psi :U\longrightarrow W and a continuous map \lambda :D^k\longrightarrow X(W)^H such that \lambda |_{\partial D^k}=X(\psi )^H\circ (\lambda ^{\prime })^H\circ \bar{\chi } and f(W)^H\circ \lambda is homotopic, relative \partial D^k, t...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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ed6b1e88bc48f9625ad2f9d4b40f7204d0d9fd7a
subsection
22
1,121
Orthogonal spaces and global equivalences
Lemma REF (or rather its G-equivariant generalization) applies to these homotopies, so instead of the original lifting problem we may solve the homotopic lifting problem@C=15mm{ A[r]^-{\alpha ^{\prime }} [d]_{\text{incl}} & X(V_n)[r]^-{i_n}[d]_{f(V_n)} & \operatorname{tel}_i X(V_i) [d]^{\operatorname{tel}_i f(V_i)} \\...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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d5c21b5736fd92a3cbea021ee9365771bb1274bb
subsection
23
1,121
Orthogonal spaces and global equivalences
But there is a G-equivariant homotopy H:X(V_n)\times [0,1]\longrightarrow \operatorname{tel}_i X(V_i) between i_m\circ X(i) and i_n, and a similar homotopy K:Y(V_n)\times [0,1]\longrightarrow \operatorname{tel}_i Y(V_i) for Y instead of X. These homotopies satisfyK\circ (f(V_n)\times [0,1]) \ = \ (\operatorname{tel}_i ...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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168314cbea743c79f9aada86bc166cdf75893054
subsection
24
1,121
Orthogonal spaces and global equivalences
The following diagram commutes@C=14mm{ X(V_n)^G [r]_-{\text{can}} [d]_{f(V_n)^G} @/^1pc/[rrr]^(.3){X(\text{incl})^G}& \operatorname{tel}_{[0,n]} X(V_i)^G [r]_-{\text{incl}} [d]_{\operatorname{tel}f(V_i)^G} & \operatorname{tel}_{[0,m]} X(V_i)^G [r]_-{\text{proj}} [d]^{\operatorname{tel}f(V_i)^G} & X(V_m)^G [d]^{f(V_m)^G...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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ec27211af8299f4f64adef45b958bd26209f3694
subsection
25
1,121
Orthogonal spaces and global equivalences
So every homotopy equivalence is in particular a strong level equivalence. By the following proposition, strong level equivalences are global equivalences.A continuous map \varphi :A\longrightarrow B is a closed embeddingclosed embeddingembedding!closed|seeclosed embedding if it is injective and a closed map. Such a ma...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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4f4e202cb03b77f07edee3178115c52736c4c812
subsection
26
1,121
Orthogonal spaces and global equivalences
If the morphisms \alpha ,\beta and \gamma are global equivalences, then so is the induced morphism of pushouts \gamma \cup \beta \ : \ C\cup _A B \ \longrightarrow \ C^{\prime }\cup _{A^{\prime }} B^{\prime }\ . Let { A [r]^-f [d]_g & B [d]^h\\ C [r]_-k & D } be a pushout square of orthogonal spaces such that f is...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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99db3041082aab4352b34dbe7bafcf3cdff73340
subsection
27
1,121
Orthogonal spaces and global equivalences
Since f is a global equivalence, the equivariant lifting problem (X(\varphi )\circ \alpha ,\lambda ) has a solution (\psi :W\longrightarrow U,\, \lambda ^{\prime }:B\longrightarrow X(U)) such that\lambda ^{\prime }|_A\ =\ X(\psi )\circ X(\varphi )\circ \alphaand such that f(U)\circ \lambda ^{\prime } is G-homotopic to ...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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0587b2d3cb1901f5bad383a5a63cfdb398f1e4a5
subsection
28
1,121
Orthogonal spaces and global equivalences
So there is a commutative diagram{ X[r]^-i [d]_f & \bar{X}[r]^-r[d]^g & X[d]^f \\ Y [r]_-j & \bar{Y} [r]_-s & Y}such that r i=\operatorname{Id}_X and s j=\operatorname{Id}_Y. We let G be a compact Lie group, V a G-representation, (B,A) a finite G-CW-pair and \alpha :A\longrightarrow X(V) and \beta :B\longrightarrow Y(V...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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23b8f264d49472aefc4b20a48272c68003ae21cf
subsection
29
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Orthogonal spaces and global equivalences
But this is straightforward: we let G be a compact Lie group, V a G-representation, (B,A) a finite G-CW-pair and \alpha :A\longrightarrow (X\times Z)(V) and \beta :B\longrightarrow (Y\times Z)(V) continuous G-maps such that (f\times Z)(V)\circ \alpha =\beta |_A. Because(X\times Z)(V) \ = \ X(V) \times Z(V)and similarly...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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c461d70eddb044bf7ddf0f5201ed66d03eeb941b
subsection
30
1,121
Orthogonal spaces and global equivalences
Moreover, the relation \psi _n(V)\circ \bar{\alpha }=\bar{\beta }|_A:A\longrightarrow Y_n(V) holds because it holds after composition with the injective map Y_n(V)\longrightarrow Y_\infty (V).Since \psi _n is a global equivalence, there is a G-equivariant linear isometric embedding \varphi :V\longrightarrow W and a con...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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b89ac35d2daaed035cbf05531fb59c1565d066bf
subsection
31
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Orthogonal spaces and global equivalences
Since \alpha , \beta and \gamma are global equivalences, the three vertical maps in the following commutative diagram of G-spaces are G-weak equivalences, by Proposition REF :@C=15mm{ \operatorname{tel}_i C(V_i) [d]_{\operatorname{tel}\gamma (V_i)} & \operatorname{tel}_i A(V_i) [l]_-{\operatorname{tel}g(V_i)} [d]^{\ope...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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821cf42e435743b5f04a436db90ffd9186725710
subsection
32
1,121
Orthogonal spaces and global equivalences
Since f is a global equivalence, there is a G-equivariant linear isometric embedding \varphi :V\longrightarrow W and a continuous G-map \lambda :B\longrightarrow X(W) such that \lambda |_A=X(\varphi )\circ k(V)\circ \alpha and such that f(W)\circ \lambda is G-homotopic, relative to A, to Y(\varphi )\circ h(V)\circ \be...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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4fb2b97dc34e6974a10ea1c6b5b5d68fff7a5bbd
subsection
33
1,121
Orthogonal spaces and global equivalences
Now we can choose a lift H^{\prime } in the square@C30mm{ B\times 1\cup _{A\times 1} A\times [0,1][d]_\sim [r]^-{\lambda \cup K^{\prime }} & X(W) @{->>}[d]^{f(W)} \\ B\times [0,1] [r]_-H @{-->}[ur]_{H^{\prime }} & Y(W) }where K^{\prime }:A\times [0,1]\longrightarrow X(W) is the constant homotopy from X(\varphi )\circ k...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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2fbe456a47bacb6dd5a12ceafd3a915102416092
subsection
34
1,121
Orthogonal spaces and global equivalences
The unique morphism from the initial (i.e., empty) to a terminal orthogonal space is not a global equivalence.The following proposition provides a lot of flexibility for changing an orthogonal space into a globally equivalent one by modifying the input variable. We will use it multiple times in this book.Theorem 1.10 ...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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43dd10a0293fa80dc92d700b3caecfbf4ca583b9
subsection
35
1,121
Orthogonal spaces and global equivalences
Then \beta |_A=Y(i_V)\circ \alpha by hypothesis, and we claim that Y(i_{F(V)})\circ \beta is G-homotopic to Y(F(i_V))\circ \beta = (Y\circ F)(i_V)\circ \beta , relative A; granting this for the moment, we conclude that the pair (i_V:V\longrightarrow F(V), \beta ) solves the lifting problem.It remains to construct the ...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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363aa62241c5361aa4b9f331fd9d2834582e5e18
subsection
36
1,121
Orthogonal spaces and global equivalences
Y)(V)\ = \ Y(V\otimes W)\ .Here, and in the rest of the book, we endow the tensor product V\otimes W of two inner product spaces V and W with the inner product characterized by\langle v\otimes w, \bar{v}\otimes \bar{w}\rangle \ = \ \langle v, \bar{v}\rangle \cdot \langle w, \bar{w}\ranglefor all v,\bar{v}\in V and w,\b...
{ "cite_spans": [ { "arxiv_id": "", "doi": "10.1007/978-3-642-66243-0", "end": 2172, "openalex_id": "https://openalex.org/W1515431404", "raw": "A. A. Kirillov, Elements of the theory of representations. Translated from the Russian by E. Hewitt. Grundlehren der Mathematischen Wissensc...
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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2a1d3c04f2eea40364fbdc55fe18d62e1e13f1c8
subsection
37
1,121
Orthogonal spaces and global equivalences
By Schur's lemma, the endomorphism algebra \operatorname{Hom}_{\mathbb {R}}^G(\lambda ,\lambda ) is a finite-dimensional skew-field extension of {\mathbb {R}}, hence isomorphic to {\mathbb {R}}, {\mathbb {C}} or {\mathbb {H}}.If \operatorname{Hom}_{\mathbb {R}}^G(\lambda ,\lambda ) is isomorphic to {\mathbb {R}}, then ...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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9bb2bccfb40635802533898ecd3c39406e95e626
subsection
38
1,121
Orthogonal spaces and global equivalences
Since there are only countably many isomorphism classes of irreducible orthogonal G-representations, a complete G-universe exists.Remark 1.13 We let H be a closed subgroup of a compact Lie group G. We will frequently use that the underlying H-representation of a complete G-universe {\mathcal {U}} is a complete H-unive...
{ "cite_spans": [ { "arxiv_id": "", "doi": "", "end": 486, "openalex_id": "https://openalex.org/W324411233", "raw": "R. S. Palais, The classification of G-spaces. Mem. Amer. Math. Soc. 36 (1960), iv+72 pp.", "source_ref_id": "7df74b609a79fe221dcafd5e7b7c46c0284c6a5c", "st...
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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f26b35bbbc0dd21f220adeca987a5af4a54d0f26
subsection
39
1,121
Orthogonal spaces and global equivalences
Then {\mathcal {U}}_G is filtered by the finite sums n\cdot \rho _G, and we getY({\mathcal {U}}_G)\ = \ \operatorname{colim}_n \, Y(n\cdot \rho _G) \ ,where the colimit is taken along the inclusions n\cdot \rho _G\longrightarrow (n+1)\cdot \rho _G that miss the last summand.Definition 1.16 An orthogonal space Y is clos...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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6e0de220d3792ff5959a6e442e1e3c4fed76adfe
subsection
40
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Orthogonal spaces and global equivalences
We turn these two actions into a single left action of the group K\times G by defining((k,g)\cdot \varphi )(v) \ = \ k\cdot \varphi (g^{-1} \cdot v)for \varphi \in {\mathbf {L}}(V,{\mathcal {U}}) and (k,g)\in K\times G. We recall that a continuous (K\times G)-equivariant map is a (K\times G)-cofibration if it has the r...
{ "cite_spans": [ { "arxiv_id": "", "doi": "10.1007/bf01456063", "end": 1564, "openalex_id": "https://openalex.org/W2156908593", "raw": "S. Illman, The equivariant triangulation theorem for actions of compact Lie groups. Math. Ann. 262 (1983), 487–501.", "source_ref_id": "1095c...
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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02ff11c217eee440b4c9cb3d16c29093e8b654da
subsection
41
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Orthogonal spaces and global equivalences
The map{\mathbf {L}}(V,{\mathbb {R}}^m)\ \longrightarrow \ {\mathbf {L}}(V,{\mathbb {R}}^{m+n}) \ ,induced by the embedding {\mathbb {R}}^m\longrightarrow {\mathbb {R}}^{m+n} as the first m coordinates, is a homeomorphism from {\mathbf {L}}(V,{\mathbb {R}}^m) onto the N-fixed points of {\mathbf {L}}(V,{\mathbb {R}}^{m+...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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1c8026eac1a2baea3c072acbb0d78dfda019a9f1
subsection
42
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Orthogonal spaces and global equivalences
Part (i) then implies that {\mathbf {L}}(V,{\mathcal {U}}) is (K\times G)-cofibrant and {\mathbf {L}}(V,{\mathcal {U}})/G is K-cofibrant.The following fundamental contractibility property goes back, at least, to Boardman and Vogt . The equivariant version that we need can be found in .Proposition 1.21 Let G be a compa...
{ "cite_spans": [ { "arxiv_id": "", "doi": "10.1007/bfb0067747", "end": 231, "openalex_id": "https://openalex.org/W200131003", "raw": "J. M. Boardman, R. M. Vogt, Homotopy-everything H-spaces. Bull. Amer. Math. Soc. 74 (1968), 1117–1122.", "source_ref_id": "d275e806ccca6bba71a0...
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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23ce341685b57af94b831492f73f2c53195ecf69
subsection
43
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Orthogonal spaces and global equivalences
The space {\mathbf {L}}(V,{\mathcal {U}}) comes with a (G\times G)-action as in (REF ), and it is (G\times G)-cofibrant by Proposition REF  (ii). Then {\mathbf {L}}(V,{\mathcal {U}}) is also cofibrant as a G-space for the diagonal action, by Proposition REF  (i). Since {\mathbf {L}}(V,{\mathcal {U}}) is G-cofibrant and...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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2275f2d12eb8a60f6bb42ddfff7b7aa85fa9ecdd
subsection
44
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Orthogonal spaces and global equivalences
Indeed, the map f^\flat (W) is the composite{\mathbf {L}}(V,W) \times _G A \ \xrightarrow{} \ {\mathbf {L}}(V,W) \times _G Y(V) \ \xrightarrow{} \ Y(W)\ .Example 1.24 For every compact Lie group G, every G-representation V and every G-space A the semifree orthogonal space {\mathbf {L}}_{G,V} A is closed.orthogonal spa...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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4bcfa61ad0174e7719291e4e709e868ee3d2ca24
subsection
45
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Orthogonal spaces and global equivalences
Since \Gamma \cap (1\times G)=\lbrace (1,1)\rbrace , every element l\in L then has a unique preimage (l,\alpha (l)) under the projection, and the assignment l\mapsto \alpha (l) is a continuous homomorphism from L to G whose graph is \Gamma .We recall that a universal G-spaceuniversal space!for a set of subgroups for a ...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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014801fdf8985f46e657a3763e7164bbc3277362
subsection
46
1,121
Orthogonal spaces and global equivalences
On the other hand, if \Gamma \cap (1\times G)=\lbrace (1,1)\rbrace , then \Gamma is the graph of a unique continuous homomorphism \alpha :L\longrightarrow G, where L is the projection of \Gamma to K. Then{\mathbf {L}}(V,{\mathcal {U}}_K)^\Gamma \ = \ {\mathbf {L}}^L(\alpha ^* V, {\mathcal {U}}_K)is the space of L-equiv...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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c4c45b00a4a59da29cbaeedb049a90896ef74125
subsection
47
1,121
Orthogonal spaces and global equivalences
Indeed, if V and \bar{V} are two faithful G-representations, then V\oplus \bar{V} is yet another one, and the two restriction morphisms{\mathbf {L}}_{G,V}\ \xleftarrow{}\ {\mathbf {L}}_{G,V\oplus \bar{V}}\ \xrightarrow{}\ {\mathbf {L}}_{G,\bar{V}}are global equivalences by Proposition REF  (ii).Example 1.28 global clas...
{ "cite_spans": [ { "arxiv_id": "", "doi": "10.1016/s0079-8169(08)x6007-6", "end": 1932, "openalex_id": "https://openalex.org/W1515066108", "raw": "T. tom Dieck, Transformation Groups. De Gruyter Studies in Mathematics, 8. Walter de Gruyter & Co., Berlin, 1987. x+312 pp.", "sou...
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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5ae345867c1f08d48652aaa4a522d3275d7b469d
subsection
48
1,121
Orthogonal spaces and global equivalences
Indeed, the total space {\mathbf {L}}(V,{\mathcal {U}}_K) is homeomorphic to the Stiefel manifold of \dim (V)-frames in {\mathbb {R}}^\infty , and hence it admits a CW-structure. Every CW-complex is a normal Hausdorff space (see for example or ), hence completely regular. So {\mathbf {L}}(V,{\mathcal {U}}_K) is complet...
{ "cite_spans": [ { "arxiv_id": "", "doi": "", "end": 273, "openalex_id": "https://openalex.org/W3040586665", "raw": "A. Hatcher, Algebraic topology. Cambridge University Press, Cambridge, 2002. xii+544 pp.", "source_ref_id": "aa1a862d9078340b2f04e22c07488ba39f0e8d42", "s...
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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9208ab6e46752e28a1cffacb239abaecbbbe32e9
subsection
49
1,121
Orthogonal spaces and global equivalences
So we are done if we can show that q:{\mathbf {L}}(V,{\mathcal {U}}_K)\longrightarrow {\mathbf {L}}(V,{\mathcal {U}}_K)/G is a universal (K,G)-principal bundle in the above sense.Universal (K,G)-principal bundles can be built in different ways; the most common construction is a version of Milnor's infinite join , see f...
{ "cite_spans": [ { "arxiv_id": "", "doi": "10.2307/1970012", "end": 336, "openalex_id": "https://openalex.org/W4237188359", "raw": "J. Milnor, Construction of universal bundles. II. Ann. of Math. (2) 63 (1956), 430–436.", "source_ref_id": "e1ca9e30dbb17b9f4dc57a9aa43c8977a528b...
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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724ebd112d92b816fd99932a383b8fe616d6e345
subsection
50
1,121
Global model structure for orthogonal spaces
In this section we establish the global model structure on the category of orthogonal spaces, see Theorem REF . Towards this aim we first discuss a `strong level model structure', which we then localize. In Proposition REF we use the global model structure to relate unstable global homotopy theory to the homotopy theo...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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016125279333ae46b4ed0908af1bc6c31fcab33d
subsection
51
1,121
Global model structure for orthogonal spaces
The extension l_m(Z) of a continuous functor Z:{\mathbf {L}}^{\le m}\longrightarrow {\mathbf {T}} is a coequalizer of the two morphisms of orthogonal spaces@C=7mm{ \coprod _{0\le j\le k\le m} {\mathbf {L}}({\mathbb {R}}^k,-)\times {\mathbf {L}}({\mathbb {R}}^j,{\mathbb {R}}^k)\times Z({\mathbb {R}}^j) \ @<-.4ex>[r] @<....
{ "cite_spans": [ { "arxiv_id": "", "doi": "", "end": 1309, "openalex_id": "https://openalex.org/W1507692549", "raw": "G. M. Kelly, Basic concepts of enriched category theory. Reprint of the 1982 original. Repr. Theory Appl. Categ. No. 10 (2005), vi+137 pp.", "source_ref_id": "...
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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de0bf4322698f6ac654785116bda0b52c24ef264
subsection
52
1,121
Global model structure for orthogonal spaces
The m-th latching spacelatching space!of an orthogonal space of Y is the O(m)-spaceL_m Y \ = \ (\operatorname{sk}^{m-1} Y)({\mathbb {R}}^m) \ ;it comes with a natural O(m)-equivariant map\nu _m=i_{m-1}({\mathbb {R}}^m)\ :\ L_m Y\ \longrightarrow \ Y({\mathbb {R}}^m) \ ,the m-th latching map.We agree to set \operatornam...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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6e06da63888ffc8b9a1354ed25dd315314933527
subsection
53
1,121
Global model structure for orthogonal spaces
We have\operatorname{sk}^0 Y \ = \ \text{const}(Y(0)) \ ,the constant orthogonal space with value Y(0); the latching map\nu _1 \ : \ L_1 Y \ = \ (\operatorname{sk}^0 Y)({\mathbb {R}}) \ = \ Y(0) \ \xrightarrow{} \ Y({\mathbb {R}})is the map induced by the unique linear isometric embedding u:0\longrightarrow {\mathbb {R...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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defd76b962dc0997cad63521aa3b421b89066c40
subsection
54
1,121
Global model structure for orthogonal spaces
The evaluation functor\operatorname{ev}_{G,V}\ : \ spc\ \longrightarrow \ G{\mathbf {T}}factors through the category {\mathbf {L}}^{\le n} as the compositespc\ \longrightarrow \ spc^{\le n} \ \xrightarrow{} \ G{\mathbf {T}}\ .So the left adjoint semifree functor {\mathbf {L}}_{G,V} can be chosen as the composite of the...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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3e851f3be8a79e15229e3485e3aaf914d6728127
subsection
55
1,121
Global model structure for orthogonal spaces
The map f({\mathbb {R}}^m):X({\mathbb {R}}^m)\longrightarrow Y({\mathbb {R}}^m) is an O(m)-weak equivalence for every m\ge 0.Clearly, condition (i) implies condition (ii), and that implies condition (iii) (because the tautological action of O(m) on {\mathbb {R}}^m is faithful). So we suppose that f({\mathbb {R}}^m) is ...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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535439febb008eef8bdd191628a95749d47cebb9
subsection
56
1,121
Global model structure for orthogonal spaces
Equivalently, for every m\ge 0 the latching map \nu _m:L_m B \longrightarrow B({\mathbb {R}}^m) is an O(m)-cofibration.We are ready to establish the strong level model structure.Proposition 2.10 The strong level equivalences, strong level fibrations and flat cofibrations form a topological cofibrantly generated model ...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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797985d6d1ddb2f0221dbea0fe8188a091bc4905
subsection
57
1,121
Global model structure for orthogonal spaces
Again by Proposition REF  (iii), J^{\operatorname{str}} detects the fibrations in the strong level model structure.The model structure is topological by Proposition REF , where we take {\mathcal {G}} as the set of orthogonal spaces L_{H,{\mathbb {R}}^m} for all m\ge 0 and all closed subgroups H of O(m), and we take {\m...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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0542daca1c8dc5093a04007b75920e5cb2ada29a
subsection
58
1,121
Global model structure for orthogonal spaces
Similarly, J^{\operatorname{str}} is a set of representatives of the isomorphism classes of morphisms{\mathbf {L}}_{G,V}\times j_k\ : \ {\mathbf {L}}_{G,V}\times D^k\times \lbrace 0\rbrace \ \longrightarrow \ {\mathbf {L}}_{G,V} \times D^k\times [0,1]for G a compact Lie group, V a faithful G-representation and k\ge 0....
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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bfc742bfe670e1214bf3a416dedfb05f2c8aa720
subsection
59
1,121
Global model structure for orthogonal spaces
Part (iii) is the special case of (ii) where K is a trivial group, using that cofibrations of spaces are in particular h-cofibrations (Corollary REF ) and hence closed embeddings (Proposition REF ).Now we proceed towards the global model structure on the category of orthogonal spaces, see Theorem REF . The weak equival...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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6204c0f7f482aab7d5726f48d7fd4ed6f120b1d3
subsection
60
1,121
Global model structure for orthogonal spaces
We consider a compact Lie group G, a faithful G-representation V, a finite G-CW-pair (B,A) and a commutative square:{ A[r]^-\alpha [d]_{\text{incl}} & X(V) [d]^{f(V)} \\ B[r]_-\beta & Y(V) }We will exhibit a continuous G-map \mu :B\longrightarrow X(V) such that \mu |_A=\alpha and such that f(V)\circ \mu is homotopic, ...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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460c93a7f448655753b765b04d04a23b2a62f099
subsection
61
1,121
Global model structure for orthogonal spaces
Since f is a global equivalence, there is a G-equivariant linear isometric embedding \varphi :V\longrightarrow W and a continuous G-map \lambda :B\longrightarrow X(W) such that \lambda |_A=X(\varphi )\circ \alpha and f(W)\circ \lambda is G-homotopic to Y(\varphi )\circ \beta relative A. Since X is static, the map X(\va...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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74a346fbe1144ad95ef1edc0ca71d70cd371af91
subsection
62
1,121
Global model structure for orthogonal spaces
Then the following two conditions are equivalent:The square of spaces \begin{aligned} @C=15mm{ \operatorname{map}(B,X)[r]^-{\operatorname{map}(j,X)} [d]_{\operatorname{map}(B,f)} & \operatorname{map}(A,X) [d]^{\operatorname{map}(A,f)} \\ \operatorname{map}(B,Y)[r]_-{\operatorname{map}(j,Y)} & \operatorname{map}(A,Y) } ...
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10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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431a06bbff96fac070e87d3e9114d248adfe2925
subsection
63
1,121
Global model structure for orthogonal spaces
Given any compact Lie group G and G-representations V and W, the restriction morphism\rho _{G,V,W} \ = \ \rho _{V,W}/G \ : \ {\mathbf {L}}_{G,V\oplus W} \ \longrightarrow \ {\mathbf {L}}_{G,V}restricts (the G-orbit of) a linear isometric embedding from V\oplus W to V. If the representation V is faithful, then this morp...
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10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
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Mathematics
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c4568ec745b50e142535b01ac13765d0008c41b0
subsection
64
1,121
Global model structure for orthogonal spaces
For the other half of the factorization axiom MC5 we apply the small object argumentsmall object argument (see for example or ) to the set J^{\operatorname{str}}\cup K. All morphisms in J^{\operatorname{str}} are flat cofibrations and strong level equivalences. Since {\mathbf {L}}_{G,V\oplus W} and {\mathbf {L}}_{G,V} ...
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10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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b5b8fa6886ef0c02146a8cb545617726946ecaeb
subsection
65
1,121
Global model structure for orthogonal spaces
Right properness follows from Proposition REF  (xii) because global fibrations are in particular strong level fibrations.The global model structure is topological by Proposition REF , with {\mathcal {G}} the set of semifree orthogonal spaces {\mathbf {L}}_{G,V} indexed by a set of representatives (G,V) of the isomorphi...
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10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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8f02aac37854cb99ccb4d69bc622feeee99fa459
subsection
66
1,121
Global model structure for orthogonal spaces
A morphism f:X\longrightarrow Y of orthogonal spaces is a fibration in the positive global model structure if and only if for every compact Lie group G, every faithful G-representation V with V\ne 0 and every equivariant linear isometric embedding \varphi :V\longrightarrow W the map f(V)^G:X(V)^G\longrightarrow Y(V)^G ...
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10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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e3d23376811d8eb06f7a9d2fc1c43b8cf13b4e60
subsection
67
1,121
Global model structure for orthogonal spaces
Then evaluation at a faithful G-representation V and the semifree functor at (G,V) are a pair of adjoint functors{ {\mathbf {L}}_{G,V}\ : \ G{\mathbf {T}}\ @<.4ex>[r] & \ spc\ : \ \operatorname{ev}_{G,V} @<.4ex>[l] }between the categories of G-spaces and orthogonal spaces. This adjoint pair is a Quillen pair with respe...
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10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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c95e73b6a1be0fc9d3ac977491f528ee5a5253b8
subsection
68
1,121
Global model structure for orthogonal spaces
So the canonical mapZ(V) \ \longrightarrow \ \operatorname{colim}_{n\ge 1}\, Z(V_n) \ = \ Z({\mathcal {U}}_G)is also a G-weak equivalence. Since Z is a globally fibrant replacement of Y, the G-space Z(V) calculates the right derived functor of \operatorname{ev}_{G,V} at Y. This exhibits a chain of two G-weak equivalenc...
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10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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a75fce6b4d1a0256ea869d342ac01a3fc1fefda3
subsection
69
1,121
Global model structure for orthogonal spaces
This data makes the functors{ (-)({\mathcal {U}}_K)\ : \ spc\quad @<.4ex>[r] & \quad K{\mathbf {T}}\ : \ R_K @<.4ex>[l] }into an adjoint pair.Proposition 2.26 Let K be a compact Lie group.The adjoint functor pair ((-)({\mathcal {U}}_K),R_K) is a Quillen pair for the global model structure of orthogonal spaces and the ...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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fecb51e7dbfff2a04e9f6c88f190f1301daf2913
subsection
70
1,121
Global model structure for orthogonal spaces
So in the commutative square@C=20mm{ (R_K(X)(V))^G[r]^-{R_K(X)(\varphi )^G} [d]_{(R_K(f)(V))^G} & (R_K(X)(V\oplus W))^G [d]^{(R_K(f)(V\oplus W))^G} \\ (R_K(Y)(V))^G[r]_-{R_K(Y)(\varphi )^G} & (R_K(Y)(V\oplus W))^G }both vertical maps are Serre fibrations and both horizontal maps are weak equivalences. The square is the...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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7940114778659f6c3c0bcd845102f04a676c9cd7
subsection
71
1,121
Global model structure for orthogonal spaces
Since R A is static (Proposition REF  (ii)) and closed, the map (R A)(\varphi ):(R A)(V)\longrightarrow (R A)(W) induced by any linear isometric embedding \varphi :V\longrightarrow W is a weak equivalence and a closed embedding. So the canonical mapA \ \cong \ \operatorname{map}({\mathbf {L}}(0,{\mathbb {R}}^\infty ),A...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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6098814c7c25d9ac178279affca9f0c9268545bf
subsection
72
1,121
Global model structure for orthogonal spaces
Then {\mathbf {L}}(W,{\mathbb {R}}^\infty ) is a universal free K-space by Proposition REF  (i). So the projection from E K\times {\mathbf {L}}(W,{\mathbb {R}}^\infty ) to the second factor is a K-weak equivalence between cofibrant K-spaces, hence a K-homotopy equivalence. So the induced map\text{const}\ : \ (R A)(W) \...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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e3c8df6ecd82eab8324df38c2d70da447e01050f
subsection
73
1,121
Global model structure for orthogonal spaces
Indeed, for every compact Lie group K the two vertical maps in the commutative square of K-spaces@C=25mm{ Y({\mathcal {U}}_K)[d]_{\text{const}}[r]^-{f({\mathcal {U}}_K)} & Z({\mathcal {U}}_K)[d]^{\text{const}}\\ \operatorname{map}(E K, Y({\mathcal {U}}_K))[r]_-{\operatorname{map}(E K, f({\mathcal {U}}_K))}^-\simeq & \o...
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10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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1e704db5b509e7820886b3eb46cf9e528e37b8eb
subsection
74
1,121
Global model structure for orthogonal spaces
Then {\mathbf {L}}_{G,V}({\mathcal {U}}_K)={\mathbf {L}}(V,{\mathcal {U}}_K)/G is a classifying space for principal (K,G)-bundles, by Proposition REF . Since G has abelian identity component, it is 1-truncated in the sense of Rezk, and so the K-space {\mathbf {L}}_{G,V}({\mathcal {U}}_K) is cofree by . So criterion (ii...
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10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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fbbabddfef13da17142d358f94e9d0f5a5af449c
subsection
75
1,121
Global model structure for orthogonal spaces
As n varies, these topological simplices assemble into a covariant functor{\mathbf {\Delta }}\ \longrightarrow {\mathbf {T}}\ , \quad [n]\ \longmapsto \ \Delta ^n\ ;the coface maps are given by(d_i)_*(t_1,\dots ,t_n) \ = \left\lbrace \begin{array}{ll} \quad (0,t_1,\dots ,t_n) & \mbox{for $i=0$,} \\ (t_1,\dots ,t_i,t_i,...
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10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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45bcbb444abbd7f11a203e0ea760ef6f06e7cbbc
subsection
76
1,121
Global model structure for orthogonal spaces
A simplicial object X can be restricted along the forgetful functor{\mathbf {\Delta }}(n)^{\operatorname{op}}_\circ \ \xrightarrow{} \ {\mathbf {\Delta }}^{\operatorname{op}} \ ,\quad (\sigma :[n]\longrightarrow [k])\ \longmapsto \ [k]\ .The n-th latching object of X is the colimit over {\mathbf {\Delta }}(n)^{\operato...
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10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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165ba247079eb1ade69192a32553ec804603714b
subsection
77
1,121
Global model structure for orthogonal spaces
Reedy's paper – albeit highly influential – remains unpublished, but an account of the Reedy model structure can for example be found in . If we form the Reedy model structure starting with the global model structure of orthogonal spaces, then the cofibrant objects are precisely the Reedy flat simplicial orthogonal spa...
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10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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825c6bbe7310953814fb367745b7a843ca4069aa
subsection
78
1,121
Monoidal structures
This section is devoted to monoidal products on the category of orthogonal spaces, with emphasis on global homotopical features. Our main focus is the box product of orthogonal spaces, a special case of a Day type convolution product, and the `good' monoidal structure for orthogonal spaces. We prove in Theorem REF that...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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b24508c2439287f58ce06448fde723a1aaa5e662
subsection
79
1,121
Monoidal structures
We will often refer to this bijection as the universal property of the box product of orthogonal spaces. universal property!of the box product Very often only the object X\boxtimes Y will be referred to as the box product, but one should keep in mind that it comes equipped with a specific, universal bimorphism.The exis...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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451e840effd151fadd8acdd4f97a4f6e5f9061b1
subsection
80
1,121
Monoidal structures
The functor X\boxtimes - preserves global equivalences.(i) For an orthogonal space Z we denote by \operatorname{sh}Z the orthogonal space defined by(\operatorname{sh}Z)(V) \ = \ Z( V\oplus V) \text{\qquad and\qquad } (\operatorname{sh}Z)(\varphi )\ = \ Z(\varphi \oplus \varphi )\ ;thus \operatorname{sh}Z is isomorphic ...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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c5c56755ef2fe4279f8b66c211ce04aee09a1cb7
subsection
81
1,121
Monoidal structures
Moreover, f_0=\lambda \circ \rho _{X,Y} and f_1=(X\boxtimes Y)\circ i_1, so this is the desired homotopy. The morphism (X\boxtimes Y)\circ i_1 is a global equivalence by Theorem REF , hence so is the morphism \lambda \circ \rho _{X,Y}.The shift functor preserves products, and under the canonical isomorphism \operatorna...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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b88e3d7aea4e484fc16a5854108fde803198cd20
subsection
82
1,121
Monoidal structures
The mapA\times B \ \xrightarrow{} \ &( {\mathbf {L}}_{G,V} A)(V)\times ({\mathbf {L}}_{K,W} B) (W)\\ \xrightarrow{}\quad &( ( {\mathbf {L}}_{G,V} A)\boxtimes ({\mathbf {L}}_{K,W} B) )(V\oplus W)is (G\times K)-equivariant, so it extends freely to a morphism of orthogonal spaces{\mathbf {L}}_{G\times K,V\oplus W}(A\times...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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8e48032498e58b3ebe1cd9c86b6ce6f58150bcff
subsection
83
1,121
Monoidal structures
A special case of this shows that the box product of two global classifying spaces is another global classifying space.global classifying space Indeed, if G acts faithfully on V and K acts faithfully on W, then the (G\times K)-action on V\oplus W is also faithful, and hence( B_{\operatorname{gl}}G) \boxtimes (B_{\opera...
{ "cite_spans": [ { "arxiv_id": "", "doi": "10.1016/j.aim.2012.07.013", "end": 1268, "openalex_id": "https://openalex.org/W1995054292", "raw": "S. Sagave, C. Schlichtkrull, Diagram spaces and symmetric spectra. Adv. Math. 231 (2012), no. 3-4, 2116–2193.", "source_ref_id": "77e2...
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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f4436d13eba013a937adff375e622ee9d5e3f124
subsection
84
1,121
Monoidal structures
The first map in (REF ) is a quotient map, and its source is compact by hypothesis (a) and because the spaces {\mathbf {L}}({\mathbb {R}}^i,V) are all compact. So the space (\operatorname{sk}^m Y)(V) is quasi-compact. Since Y(V) is Hausdorff, the map i_m(V) is a closed map. So all that remains is to show that i_m(V) is...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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82342dc1a9a7f47aa96e3940b11baedd6a2d933c
subsection
85
1,121
Monoidal structures
An element of y\in Y({\mathbb {R}}^m) is in the image of the latching map if an only if it is in the image of the map Y(U)\longrightarrow Y({\mathbb {R}}^m) for some (m-1)-dimensional subspace U of {\mathbb {R}}^m. Then the orthogonal reflection in the hyperplane U fixes y. Conversely, if y is fixed by a reflection, th...
{ "cite_spans": [ { "arxiv_id": "", "doi": "10.1007/bf01456063", "end": 2396, "openalex_id": "https://openalex.org/W2156908593", "raw": "S. Illman, The equivariant triangulation theorem for actions of compact Lie groups. Math. Ann. 262 (1983), 487–501.", "source_ref_id": "1095c...
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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a0e32f09c3e721d50fc89d13465ab96015e18f22
subsection
86
1,121
Monoidal structures
Finally, if a pair(\varphi ,\psi ) \ \in \ {\mathbf {L}}(V,U)\times {\mathbf {L}}(W,U)is fixed by the reflection in some hyperplane U^{\prime } of U, then the images of \varphi and \psi are contained in U^{\prime }, and hence (\varphi ,\psi ) lies in the image of {\mathbf {L}}(V,U^{\prime })\times {\mathbf {L}}(W,U^{\p...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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e62a45bcb1e789a284727788815499cbdf33fc34
subsection
87
1,121
Monoidal structures
The next construction introduces the orthogonal space {\mathbf {L}}^{\mathbb {C}}_{G,W} for a unitary G-representation W. In contrast to their orthogonal cousins {\mathbf {L}}_{G,V}, the unitary analogs are not representable nor semifree in any sense. However, the unitary versions also enjoy various useful properties, ...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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24cf197dae171d3265ef303076d75725874584b4
subsection
88
1,121
Monoidal structures
We define the orthogonal space {\mathbf {L}}^{\mathbb {C}}_{G,W} by{\mathbf {L}}^{\mathbb {C}}_{G,W}(V) \ = \ \ {\mathbf {L}}^{\mathbb {C}}(W,V_{\mathbb {C}}) / G\ .We define a morphism of orthogonal spacesf_{G,W} \ : \ {\mathbf {L}}_{G, u W} \ \longrightarrow \ {\mathbf {L}}^{\mathbb {C}}_{G, W}as follows. The mapj_W ...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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97ba56c352cee1915a7edc330b3eb0bb1f829dbc
subsection
89
1,121
Monoidal structures
Since {\mathbb {C}}\otimes _{\mathbb {R}}{\mathcal {U}}_K is a complete complex G-universe, the complex analog of Proposition REF  (i), proved in much the same way, shows that the target of \tilde{f} is also such a universal space for the same family of subgroups of K\times G. So \tilde{f} is a (K\times G)-equivariant ...
{ "cite_spans": [ { "arxiv_id": "", "doi": "10.1007/bf01456063", "end": 926, "openalex_id": "https://openalex.org/W2156908593", "raw": "S. Illman, The equivariant triangulation theorem for actions of compact Lie groups. Math. Ann. 262 (1983), 487–501.", "source_ref_id": "1095cd...
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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8f1045198d4d8fbc6bd25dbac6658a6eb9e142e2
subsection
90
1,121
Monoidal structures
The maps{\mathbf {L}}^{\mathbb {C}}(W,V_{\mathbb {C}})/G \times {\mathbf {L}}^{\mathbb {C}}(U,V^{\prime }_{\mathbb {C}})/K \ &\longrightarrow \ {\mathbf {L}}^{\mathbb {C}}(W\oplus U,(V\oplus V^{\prime })_{\mathbb {C}})/ ( G\times K )\\ ( \varphi \cdot G,\, \psi \cdot K ) \qquad \quad &\longmapsto \qquad (\varphi \oplus...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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47845fc2a1b1c9c5be6421f1a691c6b0e6b380e6
subsection
91
1,121
Global families
In this section we explain a variant of unstable global homotopy theory based on a global family, i.e., a class {\mathcal {F}} of compact Lie groups with certain closure properties. We introduce {\mathcal {F}}-equivalences, a relative version of global equivalences, and establish an {\mathcal {F}}-relative version of t...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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027e1ec22fbe84d53f191aa6c1e4c519e5ea15cf
subsection
92
1,121
Global families
A morphism f:X\longrightarrow Y of orthogonal spaces isan {\mathcal {F}}-level equivalenceF-level equivalence@{\mathcal {F}}-level equivalence!of orthogonal spaces if for every compact Lie group G in {\mathcal {F}} and every G-representation V the map f(V)^G:X(V)^G\longrightarrow Y(V)^G is a weak equivalence; an {\mat...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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d8f472e8fed79d5100bc8003a9598e84c2a7d8ed
subsection
93
1,121
Global families
The {\mathcal {F}}-level equivalences, {\mathcal {F}}-level fibrations and {\mathcal {F}}-cofibrations form a topological and cofibrantly generated model structure, the {\mathcal {F}}-level model structure,F-level model structure@{\mathcal {F}}-level model structure!for orthogonal spaces on the category of orthogonal s...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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41e48e1c9784e2cec555b23dd8f145b24a7fc453
subsection
94
1,121
Global families
A morphism f:X\longrightarrow Y of orthogonal spaces is an {\mathcal {F}}-equivalenceF-equivalence@{\mathcal {F}}-equivalence!of orthogonal spaces if the following condition holds: for every compact Lie group G in {\mathcal {F}}, every G-representation V, every k\ge 0 and all maps \alpha :\partial D^k\longrightarrow X(...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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2c33a2287cb36f4d4c2a3b03ee52aee20532a30b
subsection
95
1,121
Global families
For every compact Lie group G in the family {\mathcal {F}} and every exhaustive sequence \lbrace V_i\rbrace _{i\ge 1} of G-representations the induced map \operatorname{tel}_i f(V_i)\ : \ \operatorname{tel}_i X(V_i)\ \longrightarrow \ \operatorname{tel}_i Y(V_i) is a G-weak equivalence.Definition 4.6 F-global fibrati...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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56a15be741d722e4a508badd639696bee066fd25
subsection
96
1,121
Global families
Then the canonical morphism f_\infty :Y_0\longrightarrow Y_\infty to the colimit of the sequence \lbrace f_n\rbrace _{n\ge 0} is an {\mathcal {F}}-equivalence. Let { C [d]_\gamma & A [l]_-g [d]^\alpha [r]^-f & B [d]^\beta \\ C^{\prime } & A^{\prime } [l]^-{g^{\prime }}[r]_-{f^{\prime }} & B^{\prime } } be a commutat...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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5ffdced40847199593ad20e84f94d71472620a57
subsection
97
1,121
Global families
The set I_{{\mathcal {F}}} detects the acyclic fibrations in the {\mathcal {F}}-level model structure, which coincide with the acyclic fibrations in the {\mathcal {F}}-global model structure.Also in Proposition REF we defined J_{{\mathcal {F}}} as the set of all morphisms G_m j for m\ge 0 and for j in the set of gener...
{ "cite_spans": [] }
10.1017/9781108349161
1802.09382
Global homotopy theory
[ "Stefan Schwede" ]
[ "math.AT" ]
2,018
en
Mathematics
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