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import OAI.Algebra.FiniteTensor.SeparatedForms
namespace OAI
/-! Exterior reindexing, separated potentials and parity of Koszul operators. -/
noncomputable section
open scoped BigOperators
namespace PD4Tensor.Forms
noncomputable section
open scoped TensorProduct
variable (K A B σ τ : Type*) [Field K] [CommRing A] [CommRing B]
[Algebra K A] [Algebra K B]
def coordinateIsometry (e : σ ≃ τ) :
(0 : QuadraticForm K (σ → K)).IsometryEquiv (0 : QuadraticForm K (τ → K)) :=
{ LinearEquiv.funCongrLeft K K e.symm with
map_app' := by intro x; rfl }
def reindexExterior (e : σ ≃ τ) : E K σ ≃ₐ[K] E K τ :=
CliffordAlgebra.equivOfIsometry (coordinateIsometry K σ τ e)
@[simp] theorem reindexExterior_ι (e : σ ≃ τ) (v : σ → K) :
reindexExterior K σ τ e (ExteriorAlgebra.ι K v)=
ExteriorAlgebra.ι K (fun j => v (e.symm j)) := by
change CliffordAlgebra.map (coordinateIsometry K σ τ e).toIsometry (CliffordAlgebra.ι _ v)=_
rw [CliffordAlgebra.map_apply_ι]
rfl
@[simp] theorem reindexExterior_dx [DecidableEq σ] [DecidableEq τ] (e : σ ≃ τ) (i : σ) :
reindexExterior K σ τ e (dx K σ i)=dx K τ (e i) := by
rw [dx,reindexExterior_ι,dx]
congr 1
funext j
simp only [Pi.single_apply]
have h : e.symm j=i ↔ j=e i := e.symm_apply_eq
simp only [h]
theorem reindexExterior_parity (e : σ ≃ τ) (v : E K σ) :
reindexExterior K σ τ e (CliffordAlgebra.involute v)=
CliffordAlgebra.involute (reindexExterior K σ τ e v) := by
induction v using ExteriorAlgebra.induction with
| algebraMap r => simp
| ι v => simp
| add a b ha hb => simp only [map_add,ha,hb]
| mul a b ha hb => simp only [map_mul,ha,hb]
def reindexForms (e : σ ≃ τ) (f : A ≃ₐ[K] B) : Ω K A σ ≃ₐ[K] Ω K B τ :=
Algebra.TensorProduct.congr f (reindexExterior K σ τ e)
@[simp] theorem reindexForms_tmul (e : σ ≃ τ) (f : A ≃ₐ[K] B) (a : A) (v : E K σ) :
reindexForms K A B σ τ e f (a ⊗ₜ[K] v)=f a ⊗ₜ[K] reindexExterior K σ τ e v := rfl
@[simp] theorem reindexForms_scalar (e : σ ≃ τ) (f : A ≃ₐ[K] B) (a : A) :
reindexForms K A B σ τ e f (scalar K A σ a)=scalar K B τ (f a) := by
simp only [scalar,reindexForms_tmul,map_one]
theorem reindexForms_differential [Fintype σ] [DecidableEq σ] [Fintype τ] [DecidableEq τ]
(e : σ ≃ τ) (f : A ≃ₐ[K] B)
(derA : σ → A →ₗ[K] A) (derB : τ → B →ₗ[K] B)
(hder : ∀ i a, derB (e i) (f a)=f (derA i a)) (ω : Ω K A σ) :
reindexForms K A B σ τ e f (differential K A σ derA ω)=
differential K B τ derB (reindexForms K A B σ τ e f ω) := by
induction ω using TensorProduct.inductionOn with
| add a b ha hb => simp only [map_add,ha,hb]
| tmul a v =>
simp only [differential_tmul,map_sum,reindexForms_tmul,map_mul,reindexExterior_dx]
exact Fintype.sum_equiv e _ _ (fun i => by rw [hder])
theorem reindexForms_parity (e : σ ≃ τ) (f : A ≃ₐ[K] B) (ω : Ω K A σ) :
reindexForms K A B σ τ e f (parity K A σ ω)=
parity K B τ (reindexForms K A B σ τ e f ω) := by
induction ω using TensorProduct.inductionOn with
| add a b ha hb => simp only [map_add,ha,hb]
| tmul a v => simp only [parity_tmul,reindexForms_tmul,reindexExterior_parity]
end
end PD4Tensor.Forms
namespace PD4Tensor.FrobeniusTruncation
noncomputable section
variable (K σ τ : Type*) [Field K] (p : ℕ)
def coordinateEquiv (e : σ ≃ τ) : Ring K σ p ≃ₐ[K] Ring K τ p :=
AlgEquiv.ofAlgHom (rename K σ p e) (rename K τ p e.symm)
(by apply hom_ext; intro i; simp)
(by apply hom_ext; intro i; simp)
@[simp] theorem coordinateEquiv_coord (e : σ ≃ τ) (i : σ) :
coordinateEquiv K σ τ p e (coord K σ p i)=coord K τ p (e i) :=
rename_coord K σ p e i
variable [CharP K p]
theorem coordinateEquiv_derivative (e : σ ≃ τ) (i : σ) (a : Ring K σ p) :
derivative K τ p (e i) (coordinateEquiv K σ τ p e a)=
coordinateEquiv K σ τ p e (derivative K σ p i a) :=
derivative_rename K σ p e e.injective i a
end
end PD4Tensor.FrobeniusTruncation
namespace PD4Tensor.TruncatedForms
noncomputable section
open scoped TensorProduct BigOperators
open Forms FrobeniusTruncation
universe u
def sigmaHeadTail {n : ℕ} (σ : Fin (n+1) → Type u) :
((i : Fin (n+1)) × σ i) ≃ σ 0 ⊕ ((i : Fin n) × σ i.succ) where
toFun v := Fin.cases (fun x => Sum.inl x) (fun i x => Sum.inr ⟨i,x⟩) v.1 v.2
invFun := Sum.elim (fun x => ⟨0,x⟩) (fun v => ⟨v.1.succ,v.2⟩)
left_inv := by rintro ⟨i,x⟩; cases i using Fin.cases <;> rfl
right_inv := by rintro (x|⟨i,x⟩) <;> rfl
def blockSigmaEquiv : {n : ℕ} → (σ : Fin (n+1) → Type u) →
BlockCoords n σ ≃ ((i : Fin (n+1)) × σ i)
| 0, σ => {
toFun := fun x => ⟨0,x⟩
invFun := fun v => cast (congrArg σ (Fin.eq_zero v.1)) v.2
left_inv := fun _ => rfl
right_inv := by
rintro ⟨i,x⟩
have hi := Fin.eq_zero i
subst i
rfl }
| n+1, σ => (Equiv.sumCongr (Equiv.refl (σ 0))
(blockSigmaEquiv (fun i => σ i.succ))).trans (sigmaHeadTail σ).symm
@[simp] theorem blockSigmaEquiv_zero (σ : Fin 1 → Type u) (x : σ 0) :
blockSigmaEquiv σ x=⟨0,x⟩ := rfl
@[simp] theorem blockSigmaEquiv_inl {n : ℕ} (σ : Fin (n+1+1) → Type u) (x : σ 0) :
blockSigmaEquiv σ (Sum.inl x)=⟨0,x⟩ := rfl
@[simp] theorem blockSigmaEquiv_inr {n : ℕ} (σ : Fin (n+1+1) → Type u)
(x : BlockCoords n (fun i => σ i.succ)) :
blockSigmaEquiv σ (Sum.inr x)=
⟨(blockSigmaEquiv (fun i => σ i.succ) x).1.succ,
(blockSigmaEquiv (fun i => σ i.succ) x).2⟩ := rfl
variable (K : Type*) [Field K] (p : ℕ)
def sigmaSeparatedEquiv {n : ℕ} (σ : Fin (n+1) → Type u)
[∀ i, Fintype (σ i)] [∀ i, DecidableEq (σ i)] :
(⨂[K] i, Space K (σ i) p) ≃ₗ[K] Space K ((i : Fin (n+1)) × σ i) p :=
(separatedEquiv K p σ).trans
(reindexForms K _ _ _ _ (blockSigmaEquiv σ)
(coordinateEquiv K _ _ p (blockSigmaEquiv σ))).toLinearEquiv
variable [CharP K p]
theorem D_sigmaSeparated {n : ℕ} (σ : Fin (n+1) → Type u)
[∀ i, Fintype (σ i)] [∀ i, DecidableEq (σ i)] (v : ⨂[K] i, Space K (σ i) p) :
D K ((i : Fin (n+1)) × σ i) p (sigmaSeparatedEquiv K p σ v) =
sigmaSeparatedEquiv K p σ (oddTensor (fun i => (parity K (A K (σ i) p) (σ i)).toLinearMap)
(fun i => D K (σ i) p) v) := by
change differential K _ _ _ (reindexForms K _ _ _ _ _ _ (separatedEquiv K p σ v))=_
rw [←reindexForms_differential K _ _ _ _ _ _ _ _
(coordinateEquiv_derivative K _ _ p (blockSigmaEquiv σ))]
change reindexForms K _ _ _ _ _ _ (D K _ p (separatedEquiv K p σ v))=_
rw [D_separated]
rfl
end
end PD4Tensor.TruncatedForms
namespace PD4Tensor.FrobeniusTruncation
noncomputable section
variable (K σ τ υ : Type*) [Field K] (p : ℕ)
theorem rename_rename (f : σ → τ) (g : τ → υ) (a : Ring K σ p) :
rename K τ p g (rename K σ p f a)=rename K σ p (g ∘ f) a := by
have h : (rename K τ p g).comp (rename K σ p f)=rename K σ p (g ∘ f) := by
apply hom_ext
intro i
simp only [AlgHom.comp_apply,rename_coord,Function.comp_apply]
exact AlgHom.congr_fun h a
@[simp] theorem coordinateEquiv_eq_rename (e : σ ≃ τ) (a : Ring K σ p) :
coordinateEquiv K σ τ p e a=rename K σ p e a := rfl
end
end PD4Tensor.FrobeniusTruncation
namespace PD4Tensor.TruncatedForms
noncomputable section
open scoped TensorProduct BigOperators
open Forms FrobeniusTruncation
universe u
variable (K : Type*) [Field K] (p : ℕ)
def sigmaPotential {n : ℕ} (σ : Fin (n+1) → Type u)
[∀ i, Fintype (σ i)] [∀ i, DecidableEq (σ i)] (S : ∀ i, A K (σ i) p) :
A K ((i : Fin (n+1)) × σ i) p :=
∑ i, rename K (σ i) p (Sigma.mk i) (S i)
def sigmaProduct {n : ℕ} (σ : Fin (n+1) → Type u)
[∀ i, Fintype (σ i)] [∀ i, DecidableEq (σ i)] (b : ∀ i, A K (σ i) p) :
A K ((i : Fin (n+1)) × σ i) p :=
∏ i, rename K (σ i) p (Sigma.mk i) (b i)
theorem separatedPotential_reindex {n : ℕ} (σ : Fin (n+1) → Type u)
[∀ i, Fintype (σ i)] [∀ i, DecidableEq (σ i)] (S : ∀ i, A K (σ i) p) :
coordinateEquiv K _ _ p (blockSigmaEquiv σ) (separatedPotential K p σ S)=
sigmaPotential K p σ S := by
induction n with
| zero =>
change rename K (σ 0) p (Sigma.mk 0) (S 0)=
∑ i : Fin 1, rename K (σ i) p (Sigma.mk i) (S i)
rw [Fin.sum_univ_one]
| succ n ih =>
change rename K (σ 0 ⊕ BlockCoords n (fun i => σ i.succ)) p (blockSigmaEquiv σ)
(rename K (σ 0) p Sum.inl (S 0) +
rename K (BlockCoords n (fun i => σ i.succ)) p Sum.inr
(separatedPotential K p (fun i => σ i.succ) (fun i => S i.succ)))=
∑ i, rename K (σ i) p (Sigma.mk i) (S i)
rw [map_add]
erw [rename_rename,rename_rename]
rw [Fin.sum_univ_succ]
congr 1
have h := congrArg
(rename K ((i : Fin (n+1)) × σ i.succ) p
(fun v => (⟨v.1.succ,v.2⟩ : (i : Fin (n+1+1)) × σ i)))
(ih (fun i => σ i.succ) (fun i => S i.succ))
simp only [coordinateEquiv_eq_rename,sigmaPotential,map_sum,rename_rename,Function.comp_def] at h
exact h
theorem separatedProduct_reindex {n : ℕ} (σ : Fin (n+1) → Type u)
[∀ i, Fintype (σ i)] [∀ i, DecidableEq (σ i)] (b : ∀ i, A K (σ i) p) :
coordinateEquiv K _ _ p (blockSigmaEquiv σ) (separatedProduct K p σ b)=
sigmaProduct K p σ b := by
induction n with
| zero =>
change rename K (σ 0) p (Sigma.mk 0) (b 0)=
∏ i : Fin 1, rename K (σ i) p (Sigma.mk i) (b i)
rw [Fin.prod_univ_one]
| succ n ih =>
change rename K (σ 0 ⊕ BlockCoords n (fun i => σ i.succ)) p (blockSigmaEquiv σ)
(rename K (σ 0) p Sum.inl (b 0) *
rename K (BlockCoords n (fun i => σ i.succ)) p Sum.inr
(separatedProduct K p (fun i => σ i.succ) (fun i => b i.succ)))=
∏ i, rename K (σ i) p (Sigma.mk i) (b i)
rw [map_mul]
erw [rename_rename,rename_rename]
rw [Fin.prod_univ_succ]
congr 1
have h := congrArg
(rename K ((i : Fin (n+1)) × σ i.succ) p
(fun v => (⟨v.1.succ,v.2⟩ : (i : Fin (n+1+1)) × σ i)))
(ih (fun i => σ i.succ) (fun i => b i.succ))
simp only [coordinateEquiv_eq_rename,sigmaProduct,map_prod,rename_rename,Function.comp_def] at h
exact h
variable [CharP K p]
theorem reindex_koszul (σ τ : Type*) [Fintype σ] [DecidableEq σ]
[Fintype τ] [DecidableEq τ] (e : σ ≃ τ) (S : A K σ p) (ω : Space K σ p) :
reindexForms K (A K σ p) (A K τ p) σ τ e (coordinateEquiv K σ τ p e)
(koszul K σ p S ω)=
koszul K τ p (coordinateEquiv K σ τ p e S)
(reindexForms K (A K σ p) (A K τ p) σ τ e (coordinateEquiv K σ τ p e) ω) := by
simp only [koszul,LinearMap.mulLeft_apply,map_mul,D,
reindexForms_differential K (A K σ p) (A K τ p) σ τ e (coordinateEquiv K σ τ p e)
(derivative K σ p) (derivative K τ p) (coordinateEquiv_derivative K σ τ p e),
reindexForms_scalar]
omit [CharP K p] in
theorem reindex_mulScalar (σ τ : Type*) [Fintype σ] [DecidableEq σ]
[Fintype τ] [DecidableEq τ] (e : σ ≃ τ) (b : A K σ p) (ω : Space K σ p) :
reindexForms K (A K σ p) (A K τ p) σ τ e (coordinateEquiv K σ τ p e)
(mulScalar K σ p b ω)=
mulScalar K τ p (coordinateEquiv K σ τ p e b)
(reindexForms K (A K σ p) (A K τ p) σ τ e (coordinateEquiv K σ τ p e) ω) := by
simp only [mulScalar,LinearMap.mulLeft_apply,map_mul,reindexForms_scalar]
theorem koszul_sigmaSeparated {n : ℕ} (σ : Fin (n+1) → Type u)
[∀ i, Fintype (σ i)] [∀ i, DecidableEq (σ i)]
(S : ∀ i, A K (σ i) p) (v : ⨂[K] i, Space K (σ i) p) :
koszul K ((i : Fin (n+1)) × σ i) p (sigmaPotential K p σ S)
(sigmaSeparatedEquiv K p σ v)=
sigmaSeparatedEquiv K p σ
(oddTensor (fun i => (parity K (A K (σ i) p) (σ i)).toLinearMap)
(fun i => koszul K (σ i) p (S i)) v) := by
rw [←separatedPotential_reindex K p σ S]
change koszul K _ p _
(reindexForms K (A K (BlockCoords n σ) p) (A K ((i : Fin (n+1)) × σ i) p)
_ _ (blockSigmaEquiv σ) (coordinateEquiv K _ _ p (blockSigmaEquiv σ))
(separatedEquiv K p σ v))=_
rw [←reindex_koszul,koszul_separated]
rfl
omit [CharP K p] in
theorem mulScalar_sigmaSeparated {n : ℕ} (σ : Fin (n+1) → Type u)
[∀ i, Fintype (σ i)] [∀ i, DecidableEq (σ i)]
(b : ∀ i, A K (σ i) p) (v : ⨂[K] i, Space K (σ i) p) :
mulScalar K ((i : Fin (n+1)) × σ i) p (sigmaProduct K p σ b)
(sigmaSeparatedEquiv K p σ v)=
sigmaSeparatedEquiv K p σ
(PiTensorProduct.map (fun i => mulScalar K (σ i) p (b i)) v) := by
rw [←separatedProduct_reindex K p σ b]
change mulScalar K _ p _
(reindexForms K (A K (BlockCoords n σ) p) (A K ((i : Fin (n+1)) × σ i) p)
_ _ (blockSigmaEquiv σ) (coordinateEquiv K _ _ p (blockSigmaEquiv σ))
(separatedEquiv K p σ v))=_
rw [←reindex_mulScalar,mulScalar_separated]
rfl
end
end PD4Tensor.TruncatedForms
namespace PD4Tensor.TruncatedForms
noncomputable section
open Forms FrobeniusTruncation
variable (K σ : Type*) [Field K] [Fintype σ] [DecidableEq σ] (p : ℕ)
[CharP K p]
theorem koszul_parity (S : A K σ p) (ω : Space K σ p) :
koszul K σ p S (parity K (A K σ p) σ ω)=
-parity K (A K σ p) σ (koszul K σ p S ω) := by
change D K σ p (scalar K (A K σ p) σ S) * parity K (A K σ p) σ ω =
-parity K (A K σ p) σ (D K σ p (scalar K (A K σ p) σ S) * ω)
rw [map_mul,D,differential_scalar,parity_oneForm,neg_mul,neg_neg]
omit [Fintype σ] [DecidableEq σ] [CharP K p] in
theorem mulScalar_parity (b : A K σ p) (ω : Space K σ p) :
mulScalar K σ p b (parity K (A K σ p) σ ω)=
parity K (A K σ p) σ (mulScalar K σ p b ω) := by
change scalar K (A K σ p) σ b * parity K (A K σ p) σ ω=
parity K (A K σ p) σ (scalar K (A K σ p) σ b * ω)
rw [map_mul,parity_scalar]
@[simp] theorem koszul_zero : koszul K σ p 0=0 := by
apply LinearMap.ext
intro ω
change D K σ p (scalar K (A K σ p) σ 0) * ω=0
rw [scalar_zero,map_zero,zero_mul]
omit [Fintype σ] [DecidableEq σ] [CharP K p] in
@[simp] theorem mulScalar_one : mulScalar K σ p 1=LinearMap.id := by
apply LinearMap.ext
intro ω
change scalar K (A K σ p) σ 1 * ω=ω
rw [scalar_one,one_mul]
end
end PD4Tensor.TruncatedForms
namespace PD4Tensor
noncomputable section
open scoped TensorProduct BigOperators
variable {K ι : Type*} [Field K] [Fintype ι] [LinearOrder ι]
variable {V : ι → Type*} [∀ i, AddCommGroup (V i)] [∀ i, Module K (V i)]
omit [Fintype ι] in
theorem oddCoordinate_congr_at (g f h : ∀ i,V i →ₗ[K] V i) (i : ι)
(hh : f i=h i) : oddCoordinate g f i=oddCoordinate g h i := by
funext j
by_cases hji : j=i
· subst j; simp only [oddCoordinate,lt_self_iff_false,ite_false,ite_true,hh]
· simp only [oddCoordinate,hji,ite_false]
theorem oddTensor_single (g f : ∀ i,V i →ₗ[K] V i) (i : ι) :
oddTensor g (Pi.single i (f i))=PiTensorProduct.map (oddCoordinate g f i) := by
classical
unfold oddTensor
rw [Finset.sum_eq_single i]
· rw [oddCoordinate_congr_at g (Pi.single i (f i)) f i (by simp)]
· intro j _ hji
apply PiTensorProduct.ext
apply MultilinearMap.ext
intro v
simp only [LinearMap.compMultilinearMap_apply,PiTensorProduct.map_tprod,LinearMap.zero_apply]
apply (PiTensorProduct.tprod K).map_coord_zero j
simp [oddCoordinate,hji]
· intro hi; exact (hi (Finset.mem_univ i)).elim
end
end PD4Tensor
end
end OAI
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