Linear equivalences of tensor products as isometries #

These results are separate from the definition of QuadraticForm.tmul as that file is very slow.

Main definitions #

QuadraticForm.Isometry.tmul: TensorProduct.map as a QuadraticForm.Isometry
QuadraticForm.tensorComm: TensorProduct.comm as a QuadraticForm.IsometryEquiv
QuadraticForm.tensorAssoc: TensorProduct.assoc as a QuadraticForm.IsometryEquiv
QuadraticForm.tensorRId: TensorProduct.rid as a QuadraticForm.IsometryEquiv
QuadraticForm.tensorLId: TensorProduct.lid as a QuadraticForm.IsometryEquiv

@[simp]

theorem QuadraticForm.tmul_comp_tensorMap {R : Type uR} {M₁ : Type uM₁} {M₂ : Type uM₂} {M₃ : Type uM₃} {M₄ : Type uM₄} [CommRing R] [AddCommGroup M₁] [AddCommGroup M₂] [AddCommGroup M₃] [AddCommGroup M₄] [Module R M₁] [Module R M₂] [Module R M₃] [Module R M₄] [Invertible 2] {Q₁ : QuadraticForm R M₁} {Q₂ : QuadraticForm R M₂} {Q₃ : QuadraticForm R M₃} {Q₄ : QuadraticForm R M₄} (f : Q₁ →qᵢ Q₂) (g : Q₃ →qᵢ Q₄) :

(Q₂.tmul Q₄).comp (TensorProduct.map f.toLinearMap g.toLinearMap) = Q₁.tmul Q₃

source

@[simp]

theorem QuadraticForm.tmul_tensorMap_apply {R : Type uR} {M₁ : Type uM₁} {M₂ : Type uM₂} {M₃ : Type uM₃} {M₄ : Type uM₄} [CommRing R] [AddCommGroup M₁] [AddCommGroup M₂] [AddCommGroup M₃] [AddCommGroup M₄] [Module R M₁] [Module R M₂] [Module R M₃] [Module R M₄] [Invertible 2] {Q₁ : QuadraticForm R M₁} {Q₂ : QuadraticForm R M₂} {Q₃ : QuadraticForm R M₃} {Q₄ : QuadraticForm R M₄} (f : Q₁ →qᵢ Q₂) (g : Q₃ →qᵢ Q₄) (x : TensorProduct R M₁ M₃) :

(Q₂.tmul Q₄) ((TensorProduct.map f.toLinearMap g.toLinearMap) x) = (Q₁.tmul Q₃) x

source

noncomputable def QuadraticForm.Isometry.tmul {R : Type uR} {M₁ : Type uM₁} {M₂ : Type uM₂} {M₃ : Type uM₃} {M₄ : Type uM₄} [CommRing R] [AddCommGroup M₁] [AddCommGroup M₂] [AddCommGroup M₃] [AddCommGroup M₄] [Module R M₁] [Module R M₂] [Module R M₃] [Module R M₄] [Invertible 2] {Q₁ : QuadraticForm R M₁} {Q₂ : QuadraticForm R M₂} {Q₃ : QuadraticForm R M₃} {Q₄ : QuadraticForm R M₄} (f : Q₁ →qᵢ Q₂) (g : Q₃ →qᵢ Q₄) :

Q₁.tmul Q₃ →qᵢ Q₂.tmul Q₄

TensorProduct.map for Quadraticform.Isometrys

Equations

f.tmul g = { toLinearMap := TensorProduct.map f.toLinearMap g.toLinearMap, map_app' := ⋯ }

Instances For

source

@[simp]

theorem QuadraticForm.Isometry.tmul_apply {R : Type uR} {M₁ : Type uM₁} {M₂ : Type uM₂} {M₃ : Type uM₃} {M₄ : Type uM₄} [CommRing R] [AddCommGroup M₁] [AddCommGroup M₂] [AddCommGroup M₃] [AddCommGroup M₄] [Module R M₁] [Module R M₂] [Module R M₃] [Module R M₄] [Invertible 2] {Q₁ : QuadraticForm R M₁} {Q₂ : QuadraticForm R M₂} {Q₃ : QuadraticForm R M₃} {Q₄ : QuadraticForm R M₄} (f : Q₁ →qᵢ Q₂) (g : Q₃ →qᵢ Q₄) (x : TensorProduct R M₁ M₃) :

(f.tmul g) x = (TensorProduct.map f.toLinearMap g.toLinearMap) x

source

@[simp]

theorem QuadraticForm.tmul_comp_tensorComm {R : Type uR} {M₁ : Type uM₁} {M₂ : Type uM₂} [CommRing R] [AddCommGroup M₁] [AddCommGroup M₂] [Module R M₁] [Module R M₂] [Invertible 2] (Q₁ : QuadraticForm R M₁) (Q₂ : QuadraticForm R M₂) :

(Q₂.tmul Q₁).comp ↑(TensorProduct.comm R M₁ M₂) = Q₁.tmul Q₂

source

@[simp]

theorem QuadraticForm.tmul_tensorComm_apply {R : Type uR} {M₁ : Type uM₁} {M₂ : Type uM₂} [CommRing R] [AddCommGroup M₁] [AddCommGroup M₂] [Module R M₁] [Module R M₂] [Invertible 2] (Q₁ : QuadraticForm R M₁) (Q₂ : QuadraticForm R M₂) (x : TensorProduct R M₁ M₂) :

(Q₂.tmul Q₁) ((TensorProduct.comm R M₁ M₂) x) = (Q₁.tmul Q₂) x

source

noncomputable def QuadraticForm.tensorComm {R : Type uR} {M₁ : Type uM₁} {M₂ : Type uM₂} [CommRing R] [AddCommGroup M₁] [AddCommGroup M₂] [Module R M₁] [Module R M₂] [Invertible 2] (Q₁ : QuadraticForm R M₁) (Q₂ : QuadraticForm R M₂) :

(Q₁.tmul Q₂).IsometryEquiv (Q₂.tmul Q₁)

TensorProduct.comm preserves tensor products of quadratic forms.

Equations

Q₁.tensorComm Q₂ = { toLinearEquiv := TensorProduct.comm R M₁ M₂, map_app' := ⋯ }

Instances For

source

@[simp]

theorem QuadraticForm.tensorComm_toLinearEquiv {R : Type uR} {M₁ : Type uM₁} {M₂ : Type uM₂} [CommRing R] [AddCommGroup M₁] [AddCommGroup M₂] [Module R M₁] [Module R M₂] [Invertible 2] (Q₁ : QuadraticForm R M₁) (Q₂ : QuadraticForm R M₂) :

(Q₁.tensorComm Q₂).toLinearEquiv = TensorProduct.comm R M₁ M₂

source

@[simp]

theorem QuadraticForm.tensorComm_apply {R : Type uR} {M₁ : Type uM₁} {M₂ : Type uM₂} [CommRing R] [AddCommGroup M₁] [AddCommGroup M₂] [Module R M₁] [Module R M₂] [Invertible 2] (Q₁ : QuadraticForm R M₁) (Q₂ : QuadraticForm R M₂) (x : TensorProduct R M₁ M₂) :

(Q₁.tensorComm Q₂) x = (TensorProduct.comm R M₁ M₂) x

source

@[simp]

theorem QuadraticForm.tensorComm_symm {R : Type uR} {M₁ : Type uM₁} {M₂ : Type uM₂} [CommRing R] [AddCommGroup M₁] [AddCommGroup M₂] [Module R M₁] [Module R M₂] [Invertible 2] (Q₁ : QuadraticForm R M₁) (Q₂ : QuadraticForm R M₂) :

(Q₁.tensorComm Q₂).symm = Q₂.tensorComm Q₁

source

@[simp]

theorem QuadraticForm.tmul_comp_tensorAssoc {R : Type uR} {M₁ : Type uM₁} {M₂ : Type uM₂} {M₃ : Type uM₃} [CommRing R] [AddCommGroup M₁] [AddCommGroup M₂] [AddCommGroup M₃] [Module R M₁] [Module R M₂] [Module R M₃] [Invertible 2] (Q₁ : QuadraticForm R M₁) (Q₂ : QuadraticForm R M₂) (Q₃ : QuadraticForm R M₃) :

(Q₁.tmul (Q₂.tmul Q₃)).comp ↑(TensorProduct.assoc R M₁ M₂ M₃) = (Q₁.tmul Q₂).tmul Q₃

source

@[simp]

theorem QuadraticForm.tmul_tensorAssoc_apply {R : Type uR} {M₁ : Type uM₁} {M₂ : Type uM₂} {M₃ : Type uM₃} [CommRing R] [AddCommGroup M₁] [AddCommGroup M₂] [AddCommGroup M₃] [Module R M₁] [Module R M₂] [Module R M₃] [Invertible 2] (Q₁ : QuadraticForm R M₁) (Q₂ : QuadraticForm R M₂) (Q₃ : QuadraticForm R M₃) (x : TensorProduct R (TensorProduct R M₁ M₂) M₃) :

(Q₁.tmul (Q₂.tmul Q₃)) ((TensorProduct.assoc R M₁ M₂ M₃) x) = ((Q₁.tmul Q₂).tmul Q₃) x

source

noncomputable def QuadraticForm.tensorAssoc {R : Type uR} {M₁ : Type uM₁} {M₂ : Type uM₂} {M₃ : Type uM₃} [CommRing R] [AddCommGroup M₁] [AddCommGroup M₂] [AddCommGroup M₃] [Module R M₁] [Module R M₂] [Module R M₃] [Invertible 2] (Q₁ : QuadraticForm R M₁) (Q₂ : QuadraticForm R M₂) (Q₃ : QuadraticForm R M₃) :

((Q₁.tmul Q₂).tmul Q₃).IsometryEquiv (Q₁.tmul (Q₂.tmul Q₃))

TensorProduct.assoc preserves tensor products of quadratic forms.

Equations

Q₁.tensorAssoc Q₂ Q₃ = { toLinearEquiv := TensorProduct.assoc R M₁ M₂ M₃, map_app' := ⋯ }

Instances For

source

@[simp]

theorem QuadraticForm.tensorAssoc_toLinearEquiv {R : Type uR} {M₁ : Type uM₁} {M₂ : Type uM₂} {M₃ : Type uM₃} [CommRing R] [AddCommGroup M₁] [AddCommGroup M₂] [AddCommGroup M₃] [Module R M₁] [Module R M₂] [Module R M₃] [Invertible 2] (Q₁ : QuadraticForm R M₁) (Q₂ : QuadraticForm R M₂) (Q₃ : QuadraticForm R M₃) :

(Q₁.tensorAssoc Q₂ Q₃).toLinearEquiv = TensorProduct.assoc R M₁ M₂ M₃

source

@[simp]

theorem QuadraticForm.tensorAssoc_apply {R : Type uR} {M₁ : Type uM₁} {M₂ : Type uM₂} {M₃ : Type uM₃} [CommRing R] [AddCommGroup M₁] [AddCommGroup M₂] [AddCommGroup M₃] [Module R M₁] [Module R M₂] [Module R M₃] [Invertible 2] (Q₁ : QuadraticForm R M₁) (Q₂ : QuadraticForm R M₂) (Q₃ : QuadraticForm R M₃) (x : TensorProduct R (TensorProduct R M₁ M₂) M₃) :

(Q₁.tensorAssoc Q₂ Q₃) x = (TensorProduct.assoc R M₁ M₂ M₃) x

source

@[simp]

theorem QuadraticForm.tensorAssoc_symm_apply {R : Type uR} {M₁ : Type uM₁} {M₂ : Type uM₂} {M₃ : Type uM₃} [CommRing R] [AddCommGroup M₁] [AddCommGroup M₂] [AddCommGroup M₃] [Module R M₁] [Module R M₂] [Module R M₃] [Invertible 2] (Q₁ : QuadraticForm R M₁) (Q₂ : QuadraticForm R M₂) (Q₃ : QuadraticForm R M₃) (x : TensorProduct R M₁ (TensorProduct R M₂ M₃)) :

(Q₁.tensorAssoc Q₂ Q₃).symm x = (TensorProduct.assoc R M₁ M₂ M₃).symm x

source

theorem QuadraticForm.comp_tensorRId_eq {R : Type uR} {M₁ : Type uM₁} [CommRing R] [AddCommGroup M₁] [Module R M₁] [Invertible 2] (Q₁ : QuadraticForm R M₁) :

Q₁.comp ↑(TensorProduct.rid R M₁) = Q₁.tmul QuadraticForm.sq

source

@[simp]

theorem QuadraticForm.tmul_tensorRId_apply {R : Type uR} {M₁ : Type uM₁} [CommRing R] [AddCommGroup M₁] [Module R M₁] [Invertible 2] (Q₁ : QuadraticForm R M₁) (x : TensorProduct R M₁ R) :

Q₁ ((TensorProduct.rid R M₁) x) = (Q₁.tmul QuadraticForm.sq) x

source

noncomputable def QuadraticForm.tensorRId {R : Type uR} {M₁ : Type uM₁} [CommRing R] [AddCommGroup M₁] [Module R M₁] [Invertible 2] (Q₁ : QuadraticForm R M₁) :

(Q₁.tmul QuadraticForm.sq).IsometryEquiv Q₁

TensorProduct.rid preserves tensor products of quadratic forms.

Equations

Q₁.tensorRId = { toLinearEquiv := TensorProduct.rid R M₁, map_app' := ⋯ }

Instances For

source

@[simp]

theorem QuadraticForm.tensorRId_toLinearEquiv {R : Type uR} {M₁ : Type uM₁} [CommRing R] [AddCommGroup M₁] [Module R M₁] [Invertible 2] (Q₁ : QuadraticForm R M₁) :

Q₁.tensorRId.toLinearEquiv = TensorProduct.rid R M₁

source

@[simp]

theorem QuadraticForm.tensorRId_apply {R : Type uR} {M₁ : Type uM₁} [CommRing R] [AddCommGroup M₁] [Module R M₁] [Invertible 2] (Q₁ : QuadraticForm R M₁) (x : TensorProduct R M₁ R) :

Q₁.tensorRId x = (TensorProduct.rid R M₁) x

source

@[simp]

theorem QuadraticForm.tensorRId_symm_apply {R : Type uR} {M₁ : Type uM₁} [CommRing R] [AddCommGroup M₁] [Module R M₁] [Invertible 2] (Q₁ : QuadraticForm R M₁) (x : M₁) :

Q₁.tensorRId.symm x = (TensorProduct.rid R M₁).symm x

source

theorem QuadraticForm.comp_tensorLId_eq {R : Type uR} {M₂ : Type uM₂} [CommRing R] [AddCommGroup M₂] [Module R M₂] [Invertible 2] (Q₂ : QuadraticForm R M₂) :

Q₂.comp ↑(TensorProduct.lid R M₂) = QuadraticForm.sq.tmul Q₂

source

@[simp]

theorem QuadraticForm.tmul_tensorLId_apply {R : Type uR} {M₂ : Type uM₂} [CommRing R] [AddCommGroup M₂] [Module R M₂] [Invertible 2] (Q₂ : QuadraticForm R M₂) (x : TensorProduct R R M₂) :

Q₂ ((TensorProduct.lid R M₂) x) = (QuadraticForm.sq.tmul Q₂) x

source

noncomputable def QuadraticForm.tensorLId {R : Type uR} {M₂ : Type uM₂} [CommRing R] [AddCommGroup M₂] [Module R M₂] [Invertible 2] (Q₂ : QuadraticForm R M₂) :

(QuadraticForm.sq.tmul Q₂).IsometryEquiv Q₂

TensorProduct.lid preserves tensor products of quadratic forms.

Equations

Q₂.tensorLId = { toLinearEquiv := TensorProduct.lid R M₂, map_app' := ⋯ }

Instances For

source

@[simp]

theorem QuadraticForm.tensorLId_toLinearEquiv {R : Type uR} {M₂ : Type uM₂} [CommRing R] [AddCommGroup M₂] [Module R M₂] [Invertible 2] (Q₂ : QuadraticForm R M₂) :

Q₂.tensorLId.toLinearEquiv = TensorProduct.lid R M₂

source

@[simp]

theorem QuadraticForm.tensorLId_apply {R : Type uR} {M₂ : Type uM₂} [CommRing R] [AddCommGroup M₂] [Module R M₂] [Invertible 2] (Q₂ : QuadraticForm R M₂) (x : TensorProduct R R M₂) :

Q₂.tensorLId x = (TensorProduct.lid R M₂) x

source

@[simp]

theorem QuadraticForm.tensorLId_symm_apply {R : Type uR} {M₂ : Type uM₂} [CommRing R] [AddCommGroup M₂] [Module R M₂] [Invertible 2] (Q₂ : QuadraticForm R M₂) (x : M₂) :

Q₂.tensorLId.symm x = (TensorProduct.lid R M₂).symm x

Documentation

Mathlib.LinearAlgebra.QuadraticForm.TensorProduct.Isometries

Linear equivalences of tensor products as isometries #

Main definitions #