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