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import OAI.LinearAlgebra.MatrixMultiplication.Tensor.ComplexDotPairing
import OAI.LinearAlgebra.MatrixMultiplication.Tensor.ComplexTensorSymmetrization
import Mathlib.Tactic
namespace OAI
/-!
# The polynomial multiplication tensor
The coefficient tensor `convolution a b` represents multiplication of binary forms
of degrees `a - 1` and `b - 1`, or equivalently ordinary coefficient convolution.
The output leg has `a + b - 1` coordinates. The definitions also make sense when
an input dimension is zero, while the nonzero and full-output-support statements
use the positive dimensions assumed in Section 5 of the paper.
-/
open scoped BigOperators
namespace MatrixMultiplication.AuxiliarySeparation
open MatrixMultiplication.Foundation
/-- The tensor `C(a,b)` of Section 5, in monomial coefficient coordinates. -/
def convolution (a b : ℕ) : Tensor ℂ (Fin a) (Fin b) (Fin (a + b - 1)) :=
fun i j k => if i.val + j.val = k.val then 1 else 0
@[simp] theorem convolution_apply (a b : ℕ)
(i : Fin a) (j : Fin b) (k : Fin (a + b - 1)) :
convolution a b i j k = if i.val + j.val = k.val then 1 else 0 := rfl
@[simp] theorem convolution_ne_zero_iff {a b : ℕ}
(i : Fin a) (j : Fin b) (k : Fin (a + b - 1)) :
convolution a b i j k ≠ 0 ↔ i.val + j.val = k.val := by
simp only [convolution]
split_ifs <;> simp_all
@[simp] theorem convolution_eq_one_iff {a b : ℕ}
(i : Fin a) (j : Fin b) (k : Fin (a + b - 1)) :
convolution a b i j k = 1 ↔ i.val + j.val = k.val := by
simp only [convolution]
split_ifs <;> simp_all
@[simp] theorem convolution_eq_zero_iff {a b : ℕ}
(i : Fin a) (j : Fin b) (k : Fin (a + b - 1)) :
convolution a b i j k = 0 ↔ i.val + j.val ≠ k.val := by
simp only [convolution]
split_ifs <;> simp_all
/-- Every pair of input monomials has a valid output coordinate. -/
def convolutionOutput {a b : ℕ} (i : Fin a) (j : Fin b) : Fin (a + b - 1) :=
⟨i.val + j.val, by have hi := i.isLt; have hj := j.isLt; omega⟩
@[simp] theorem convolution_at_output {a b : ℕ} (i : Fin a) (j : Fin b) :
convolution a b i j (convolutionOutput i j) = 1 := by
simp [convolutionOutput]
/-- Every output monomial of the expected degree occurs in the product. -/
theorem convolution_output_supported {a b : ℕ} (ha : 0 < a) (hb : 0 < b)
(k : Fin (a + b - 1)) :
∃ (i : Fin a) (j : Fin b), convolution a b i j k = 1 := by
by_cases hk : k.val < a
· exact ⟨⟨k.val, hk⟩, ⟨0, hb⟩, by simp⟩
· have hk' := k.isLt
refine ⟨⟨a - 1, by omega⟩, ⟨k.val - (a - 1), by omega⟩, ?_⟩
apply (convolution_eq_one_iff _ _ _).mpr
dsimp
omega
theorem convolution_nonzero {a b : ℕ} (ha : 0 < a) (hb : 0 < b) :
convolution a b ≠ 0 := by
intro hz
have hc := congrFun (congrFun (congrFun hz ⟨0, ha⟩) ⟨0, hb⟩)
(convolutionOutput ⟨0, ha⟩ ⟨0, hb⟩)
change convolution a b ⟨0, ha⟩ ⟨0, hb⟩
(convolutionOutput ⟨0, ha⟩ ⟨0, hb⟩) = 0 at hc
rw [convolution_at_output] at hc
exact one_ne_zero hc
theorem convolution_nonzero_iff (a b : ℕ) :
convolution a b ≠ 0 ↔ 0 < a ∧ 0 < b := by
constructor
· intro h
constructor
· by_contra ha
have ha' : a = 0 := by omega
subst a
apply h
funext i
exact Fin.elim0 i
· by_contra hb
have hb' : b = 0 := by omega
subst b
apply h
funext i j
exact Fin.elim0 j
· rintro ⟨ha, hb⟩
exact convolution_nonzero ha hb
/-- Commuting the two inputs only casts the equal output dimensions. -/
theorem convolution_comm (a b : ℕ) (i : Fin a) (j : Fin b)
(k : Fin (a + b - 1)) :
convolution a b i j k =
convolution b a j i (Fin.cast (by omega) k) := by
simp only [convolution, Fin.val_cast, Nat.add_comm]
/-- The boundary tensor `C(1,b)` has the coefficient matrix of a dot product. -/
theorem convolution_one_left (b : ℕ) (i : Fin 1) (j : Fin b)
(k : Fin (1 + b - 1)) :
convolution 1 b i j k = if j.val = k.val then 1 else 0 := by
simp [convolution]
/-- The other boundary tensor has the same coordinate identity. -/
theorem convolution_one_right (a : ℕ) (i : Fin a) (j : Fin 1)
(k : Fin (a + 1 - 1)) :
convolution a 1 i j k = if i.val = k.val then 1 else 0 := by
simp [convolution]
/-- Relabel the output of `C(1,b)` by its actual dimension `b`. -/
def convolutionOneOutputEquiv (b : ℕ) : Fin b ≃ Fin (1 + b - 1) :=
finCongr (by omega)
/-- Relabel the single input coordinate of `C(1,b)` by `Unit`. -/
def convolutionOneInputEquiv : Unit ≃ Fin 1 where
toFun _ := 0
invFun _ := ()
left_inv _ := rfl
right_inv _i := Subsingleton.elim _ _
/-- `C(1,b)` is the dot-product tensor with the singleton on the first leg. -/
theorem convolution_one_left_dotPairing (b : ℕ) :
Tensor.pullback convolutionOneInputEquiv (Equiv.refl (Fin b))
(convolutionOneOutputEquiv b) (convolution 1 b) =
Tensor.cyclic (Tensor.cyclic (Tensor.dotPairing (K := ℂ) (Fin b))) := by
funext i j k
simp [Tensor.pullback, convolutionOneInputEquiv, convolutionOneOutputEquiv,
Tensor.cyclic, Tensor.dotPairing, convolution, Fin.ext_iff]
/-- Relabel the output of `C(a,1)` by its actual dimension `a`. -/
def convolutionRightOneOutputEquiv (a : ℕ) : Fin a ≃ Fin (a + 1 - 1) :=
finCongr (by omega)
/-- `C(a,1)` is the dot-product tensor with the singleton on the second leg. -/
theorem convolution_one_right_dotPairing (a : ℕ) :
Tensor.pullback (Equiv.refl (Fin a)) convolutionOneInputEquiv
(convolutionRightOneOutputEquiv a) (convolution a 1) =
Tensor.cyclic (Tensor.dotPairing (K := ℂ) (Fin a)) := by
funext i j k
simp [Tensor.pullback, convolutionOneInputEquiv, convolutionRightOneOutputEquiv,
Tensor.cyclic, Tensor.dotPairing, convolution, Fin.ext_iff, eq_comm]
/-- Contracting the coefficient tensor computes ordinary finite convolution. -/
theorem contract_convolution {a b : ℕ} (x : Fin a → ℂ) (y : Fin b → ℂ)
(k : Fin (a + b - 1)) :
Tensor.contract (convolution a b) x y k =
∑ i : Fin a, ∑ j : Fin b,
if i.val + j.val = k.val then x i * y j else 0 := by
simp [Tensor.contract, convolution, ite_mul]
end MatrixMultiplication.AuxiliarySeparation
end OAI