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import OAI.Computability.RationalHitting.QuantumSeries
namespace OAI
namespace RationalHitting.HahnMatrix
open HahnSeries Matrix
open scoped BigOperators
noncomputable section
variable {Γ R S : Type*} [AddCommGroup Γ] [LinearOrder Γ] [IsOrderedAddMonoid Γ]
[Ring R] [Ring S]
def mapCoeff (φ : R →+* S) : HahnSeries Γ R →+* HahnSeries Γ S where
toFun x := x.map φ.toZeroHom
map_zero' := HahnSeries.map_zero φ.toZeroHom
map_one' := HahnSeries.map_one φ.toMonoidWithZeroHom
map_add' _ _ := HahnSeries.map_add φ.toAddMonoidHom
map_mul' _ _ := HahnSeries.map_mul φ.toNonUnitalRingHom
lemma coeff_mul_support_superset (x y : HahnSeries Γ R) (a : Γ)
(s t : Set Γ) (hs : s.IsPWO) (ht : t.IsPWO)
(hxs : x.support ⊆ s) (hyt : y.support ⊆ t) :
(x*y).coeff a = ∑ ij ∈ Finset.antidiagonal hs ht a,
x.coeff ij.1 * y.coeff ij.2 := by
rw [HahnSeries.coeff_mul]
apply Finset.sum_subset
· intro ij hij
rw [Finset.mem_antidiagonal] at hij ⊢
exact ⟨hxs hij.1, hyt hij.2.1, hij.2.2⟩
· intro ij hij hnot
rw [Finset.mem_antidiagonal] at hij
by_cases hx : x.coeff ij.1 = 0
· simp [hx]
by_cases hy : y.coeff ij.2 = 0
· simp [hy]
exact False.elim (hnot (Finset.mem_antidiagonal.mpr ⟨hx,hy,hij.2.2⟩))
variable {ι : Type*} [Fintype ι] [DecidableEq ι]
def entry (x : HahnSeries Γ (Matrix ι ι R)) (i j : ι) : HahnSeries Γ R :=
x.map (⟨fun A => A i j, rfl⟩ : ZeroHom (Matrix ι ι R) R)
@[simp] lemma entry_coeff.{v_1, v_2, v_4} {Γ : Type v_1} {R : Type v_2}
[AddCommGroup Γ] [LinearOrder Γ] [IsOrderedAddMonoid Γ] [Ring R] {ι : Type v_4} [Fintype ι]
[DecidableEq ι] (x : HahnSeries Γ (Matrix ι ι R)) (i j : ι) (a : Γ) :
(RationalHitting.HahnMatrix.entry x i j).coeff a = x.coeff a i j := rfl
lemma entry_support.{v_1, v_2, v_4} {Γ : Type v_1} {R : Type v_2}
[AddCommGroup Γ] [LinearOrder Γ] [IsOrderedAddMonoid Γ] [Ring R] {ι : Type v_4} [Fintype ι]
[DecidableEq ι] (x : HahnSeries Γ (Matrix ι ι R)) (i j : ι) :
(RationalHitting.HahnMatrix.entry x i j).support ⊆ x.support := by
intro a ha
change x.coeff a ≠ 0
intro h
exact ha (by change x.coeff a i j = 0; rw [h]; rfl)
def split : HahnSeries Γ (Matrix ι ι R) →+* Matrix ι ι (HahnSeries Γ R) where
toFun x := entry x
map_zero' := by ext i j a; rfl
map_one' := by
ext i j a
change (1 : HahnSeries Γ (Matrix ι ι R)).coeff a i j =
(if i = j then (1 : HahnSeries Γ R) else 0).coeff a
by_cases hi : i = j <;> by_cases ha : a = 0 <;> simp [hi,ha]
map_add' x y := by ext i j a; rfl
map_mul' x y := by
ext i j a
change (x*y).coeff a i j = (∑ k, entry x i k * entry y k j).coeff a
rw [HahnSeries.coeff_mul, Matrix.sum_apply, HahnSeries.coeff_sum]
simp_rw [coeff_mul_support_superset _ _ a x.support y.support
x.isPWO_support y.isPWO_support (entry_support x i _) (entry_support y _ j)]
rw [Finset.sum_comm]
rfl
lemma split_injective : Function.Injective (split (Γ := Γ) (R := R) (ι := ι)) := by
intro x y h
ext a i j
exact congrArg (fun z : Matrix ι ι (HahnSeries Γ R) => (z i j).coeff a) h
variable {K : Type*} [Field K]
/-- Scalar series embedded as scalar matrices at each coefficient. -/
def scalarSeries : HahnSeries Γ K →+* HahnSeries Γ (Matrix ι ι K) :=
mapCoeff (algebraMap K (Matrix ι ι K))
lemma split_scalarSeries (x : HahnSeries Γ K) :
split (scalarSeries (ι := ι) x) = algebraMap (HahnSeries Γ K)
(Matrix ι ι (HahnSeries Γ K)) x := by
ext i j a
change (algebraMap K (Matrix ι ι K) (x.coeff a)) i j = _
by_cases h : i = j <;> simp [Matrix.algebraMap_matrix_apply, h, ]
lemma scalarSeries_commute (x : HahnSeries Γ K) (y : HahnSeries Γ (Matrix ι ι K)) :
scalarSeries x * y = y * scalarSeries x := by
apply split_injective
rw [map_mul, map_mul, split_scalarSeries, Algebra.commutes]
/-- The natural scalar-series algebra structure, derived through an injective
matrix realization rather than assuming commutative matrix coefficients. -/
@[instance_reducible]
def seriesAlgebra : Algebra (HahnSeries Γ K) (HahnSeries Γ (Matrix ι ι K)) :=
(scalarSeries (Γ := Γ) (K := K) (ι := ι)).toAlgebra'
(fun x y => scalarSeries_commute x y)
end
end RationalHitting.HahnMatrix
namespace RationalHitting.QuantumMatrices
open Matrix
open scoped BigOperators
noncomputable section
variable {K : Type*} [Field K] {d : ℕ} [NeZero d]
variable (χ : AddChar (ZMod d) K)
/-- The Weyl monomial D^a S^b. -/
def weyl (a b : ZMod d) : Matrix (ZMod d) (ZMod d) K :=
fun i j => if i = j+b then χ (a*i) else 0
@[simp] lemma weyl_zero.{v_1} {K : Type v_1} [Field K] {d : ℕ} [NeZero d]
(χ : AddChar (ZMod d) K) : RationalHitting.QuantumMatrices.weyl χ 0 0 = 1 := by
ext i j
simp [weyl, Matrix.one_apply]
lemma weyl_mul (a b c e : ZMod d) :
weyl χ a b * weyl χ c e = χ (-c*b) • weyl χ (a+c) (b+e) := by
classical
ext i j
rw [Matrix.mul_apply, Finset.sum_eq_single (i-b)]
· simp only [weyl, sub_add_cancel, ite_true, Matrix.smul_apply, smul_eq_mul]
have heq : i-b = j+e ↔ i = j+(b+e) := by constructor <;> intro h <;> linear_combination h
by_cases h : i = j+(b+e)
· simp only [ite_eq_left (heq.mpr h), ite_eq_left h]
rw [← AddChar.map_add_eq_mul, ← AddChar.map_add_eq_mul]
congr 1
ring
· simp [heq, h]
· intro k hk hne
have h : i ≠ k+b := by intro heq; apply hne; rw [heq]; ring
simp [weyl, h]
· simp
lemma weyl_inverse_right (a b : ZMod d) :
weyl χ a b * (χ (-a*b) • weyl χ (-a) (-b)) = 1 := by
rw [Matrix.mul_smul, weyl_mul, add_neg_cancel, add_neg_cancel, weyl_zero, smul_smul,
← AddChar.map_add_eq_mul]
have h : -a*b + -(-a)*b = 0 := by ring
rw [h, AddChar.map_zero_eq_one, one_smul]
lemma weyl_inverse_left (a b : ZMod d) :
(χ (-a*b) • weyl χ (-a) (-b)) * weyl χ a b = 1 := by
rw [Matrix.smul_mul, weyl_mul, neg_add_cancel, neg_add_cancel, weyl_zero, smul_smul,
← AddChar.map_add_eq_mul]
have h : -a*b + -a*(-b) = 0 := by ring
rw [h, AddChar.map_zero_eq_one, one_smul]
def weylUnit (a b : ZMod d) : (Matrix (ZMod d) (ZMod d) K)ˣ :=
⟨weyl χ a b, χ (-a*b) • weyl χ (-a) (-b),
weyl_inverse_right χ a b, weyl_inverse_left χ a b⟩
@[simp] lemma weylUnit_val (a b : ZMod d) : (weylUnit χ a b : Matrix _ _ K) = weyl χ a b := rfl
@[simp] lemma weylUnit_zero : weylUnit χ 0 0 = 1 := by
apply Units.ext
exact weyl_zero χ
end
end RationalHitting.QuantumMatrices
namespace RationalHitting.QuantumMatrices
open Matrix
open scoped BigOperators
noncomputable section
variable {K : Type*} [Field K] [CharZero K] {d : ℕ} [NeZero d]
variable (χ : AddChar (ZMod d) K) (hχ : χ.IsPrimitive)
def fourierCoeff (R : Matrix (ZMod d) (ZMod d) K) (a b : ZMod d) : K :=
(d : K)⁻¹ * ∑ j, χ (-a*j) * R j (j-b)
lemma orthogonality.{v_1} {K : Type v_1} [Field K] [CharZero K] {d : ℕ}
[NeZero d] (χ : AddChar (ZMod d) K) (hχ : χ.IsPrimitive) (x : ZMod d) :
∑ a, χ (a * x) = if x = 0 then ↑d else 0 := by
classical
by_cases hx : x = 0
· simp [hx, ZMod.card]
· rw [ite_eq_right hx]
simpa [AddChar.mulShift_apply, mul_comm] using AddChar.sum_eq_zero_of_ne_one (hχ hx)
include hχ in
/-- Fourier inversion on each cyclic matrix diagonal. -/
theorem fourier_reconstruction (R : Matrix (ZMod d) (ZMod d) K) :
(∑ a, ∑ b, fourierCoeff χ R a b • weyl χ a b) = R := by
classical
ext i j
simp only [Matrix.sum_apply, Matrix.smul_apply, smul_eq_mul, weyl]
simp_rw [mul_ite, mul_zero]
have heq (a : ZMod d) :
(∑ b, if i = j+b then fourierCoeff χ R a b * χ (a*i) else 0) =
fourierCoeff χ R a (i-j) * χ (a*i) := by
rw [Finset.sum_eq_single (i-j)]
· simp
· intro b hb hne
rw [ite_eq_right]
intro h
apply hne
linear_combination -h
· simp
simp_rw [heq, fourierCoeff, mul_assoc, Finset.sum_mul]
rw [← Finset.mul_sum, Finset.sum_comm]
have hc (k : ZMod d) :
(∑ a, χ (-a*k) * R k (k-(i-j)) * χ (a*i)) =
(if i = k then (d : K) else 0) * R k (k-(i-j)) := by
calc
_ = (∑ a, χ (a*(i-k))) * R k (k-(i-j)) := by
rw [Finset.sum_mul]
apply Finset.sum_congr rfl
intro a ha
rw [mul_right_comm, ← AddChar.map_add_eq_mul]
congr 2
ring
_ = _ := by simp only [orthogonality χ hχ, sub_eq_zero]
simp_rw [hc]
simp only [ite_mul, zero_mul]
rw [Finset.sum_ite_eq]
simp [Nat.cast_ne_zero.mpr (NeZero.ne d)]
end
end RationalHitting.QuantumMatrices
namespace RationalHitting.QuantumLift
open HahnSeries Matrix
open RationalHitting.QuantumSeries RationalHitting.QuantumMatrices
open scoped BigOperators
noncomputable section
variable {K : Type*} [Field K] [CharZero K] {d : ℕ} [NeZero d]
variable (χ : AddChar (ZMod d) K)
abbrev Exponents := ℤ ×ₗ ℤ
abbrev Ambient := HahnSeries Exponents (Matrix (ZMod d) (ZMod d) K)
def monomialUnit (g : Exponents) : (Matrix (ZMod d) (ZMod d) K)ˣ :=
weylUnit χ (ofLex g).1 (ofLex g).2
lemma monomialUnit_zero.{v_1} {K : Type v_1} [Field K] [CharZero K] {d : ℕ}
[NeZero d] (χ : AddChar (ZMod d) K) : RationalHitting.QuantumLift.monomialUnit χ 0 = 1 := by
simp [monomialUnit]
lemma monomialUnit_mul.{v_1} {K : Type v_1} [Field K] [CharZero K] {d : ℕ}
[NeZero d] (χ : AddChar (ZMod d) K) (g h : RationalHitting.QuantumLift.Exponents) :
∃ c : K,
(RationalHitting.QuantumLift.monomialUnit χ g : Matrix (ZMod d) (ZMod d) K) *
(RationalHitting.QuantumLift.monomialUnit χ h : Matrix (ZMod d) (ZMod d) K) =
c • (RationalHitting.QuantumLift.monomialUnit χ (g + h) : Matrix (ZMod d) (ZMod d) K) := by
refine ⟨χ (-((ofLex h).1 : ZMod d) * ((ofLex g).2 : ZMod d)), ?_⟩
simp [monomialUnit, weyl_mul]
abbrev DivisionSubring := coefficientRing (monomialUnit χ) (monomialUnit_zero χ) (monomialUnit_mul χ)
noncomputable instance : DivisionRing (DivisionSubring χ) :=
divisionRing (monomialUnit χ) (monomialUnit_zero χ) (monomialUnit_mul χ)
/-- The Fourier lift as a finite Hahn series. -/
def lift (R : Matrix (ZMod d) (ZMod d) K) : Ambient (K := K) (d := d) :=
∑ a : ZMod d, ∑ b : ZMod d,
single (toLex ((a.val : ℤ), (b.val : ℤ))) (fourierCoeff χ R a b • weyl χ a b)
lemma lift_mem (R : Matrix (ZMod d) (ZMod d) K) : lift χ R ∈ DivisionSubring χ := by
apply Subring.sum_mem
intro a ha
apply Subring.sum_mem
intro b hb
apply single_mem (monomialUnit χ) (monomialUnit_zero χ) (monomialUnit_mul χ)
apply Submodule.mem_span_singleton.mpr
refine ⟨fourierCoeff χ R a b, ?_⟩
simp [monomialUnit]
def liftD (R : Matrix (ZMod d) (ZMod d) K) : DivisionSubring χ := ⟨lift χ R, lift_mem χ R⟩
/-- The representation used in the rank-gap argument. Its coefficient field
is a commutative Hahn field; all inversion takes place inside the division
subring, never by adjoining arbitrary matrix-field scalars. -/
def representation : DivisionSubring χ →+* Matrix (ZMod d) (ZMod d) (HahnSeries Exponents K) :=
(RationalHitting.HahnMatrix.split (Γ := Exponents)).comp (DivisionSubring χ).subtype
end
end RationalHitting.QuantumLift
end OAI