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/-
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Copyright (c) 2024 Stefan Kebekus. All rights reserved.
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Released under Apache 2.0 license as described in the file LICENSE.
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Authors: Stefan Kebekus
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-/
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import Mathlib.Analysis.InnerProductSpace.PiL2
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import Mathlib.Analysis.InnerProductSpace.PiL2
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/-!
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# Canoncial Elements in Tensor Powers of Real Inner Product Spaces
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Given an `InnerProductSpace ℝ E`, this file defines two canonical tensors, which
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are relevant when for a coordinate-free definition of differential operators
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such as the Laplacian.
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* `InnerProductSpace.canonicalContravariantTensor E : E ⊗[ℝ] E →ₗ[ℝ] ℝ`. This is
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the element corresponding to the inner product.
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* If `E` is finite-dimensional, then `E ⊗[ℝ] E` is canonically isomorphic to its
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dual. Accordingly, there exists an element
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`InnerProductSpace.canonicalCovariantTensor E : E ⊗[ℝ] E` that corresponds to
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`InnerProductSpace.canonicalContravariantTensor E` under this identification.
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The theorem `InnerProductSpace.canonicalCovariantTensorRepresentation` shows
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that `InnerProductSpace.canonicalCovariantTensor E` can be computed from any
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orthonormal basis `v` as `∑ i, (v i) ⊗ₜ[ℝ] (v i)`.
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-/
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open TensorProduct
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open TensorProduct
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@ -14,26 +43,28 @@ lemma OrthonormalBasis.sum_repr'
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simp_rw [b.repr_apply_apply v]
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simp_rw [b.repr_apply_apply v]
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noncomputable def InnerProductSpace.canonicalTensor
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noncomputable def InnerProductSpace.canonicalContravariantTensor
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(E : Type u_2) [NormedAddCommGroup E] [InnerProductSpace ℝ E] [FiniteDimensional ℝ E]
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{E : Type*} [NormedAddCommGroup E] [InnerProductSpace ℝ E]
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: E ⊗[ℝ] E := by
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: E ⊗[ℝ] E →ₗ[ℝ] ℝ := TensorProduct.lift bilinFormOfRealInner
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let v := stdOrthonormalBasis ℝ E
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exact ∑ i, (v i) ⊗ₜ[ℝ] (v i)
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theorem InnerProductSpace.InvariantTensor
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noncomputable def InnerProductSpace.canonicalCovariantTensor
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(E : Type*) [NormedAddCommGroup E] [InnerProductSpace ℝ E] [FiniteDimensional ℝ E]
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(E : Type*) [NormedAddCommGroup E] [InnerProductSpace ℝ E] [FiniteDimensional ℝ E]
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(v : OrthonormalBasis (Fin (FiniteDimensional.finrank ℝ E)) ℝ E)
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: E ⊗[ℝ] E := ∑ i, ((stdOrthonormalBasis ℝ E) i) ⊗ₜ[ℝ] ((stdOrthonormalBasis ℝ E) i)
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: InnerProductSpace.canonicalTensor E = ∑ i, (v i) ⊗ₜ[ℝ] (v i) := by
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unfold InnerProductSpace.canonicalTensor
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let v₁ := stdOrthonormalBasis ℝ E
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theorem InnerProductSpace.canonicalCovariantTensorRepresentation
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(E : Type*) [NormedAddCommGroup E] [InnerProductSpace ℝ E] [FiniteDimensional ℝ E]
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[Fintype ι]
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(v : OrthonormalBasis ι ℝ E)
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: InnerProductSpace.canonicalCovariantTensor E = ∑ i, (v i) ⊗ₜ[ℝ] (v i) := by
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let w := stdOrthonormalBasis ℝ E
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conv =>
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conv =>
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right
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right
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arg 2
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arg 2
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intro i
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intro i
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rw [v₁.sum_repr' (v i)]
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rw [w.sum_repr' (v i)]
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simp_rw [TensorProduct.sum_tmul, TensorProduct.tmul_sum, TensorProduct.smul_tmul_smul]
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simp_rw [TensorProduct.sum_tmul, TensorProduct.tmul_sum, TensorProduct.smul_tmul_smul]
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conv =>
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conv =>
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@ -48,11 +79,11 @@ theorem InnerProductSpace.InvariantTensor
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arg 1
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arg 1
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arg 2
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arg 2
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intro i
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intro i
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rw [← real_inner_comm (v₁ x)]
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rw [← real_inner_comm (w x)]
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simp_rw [OrthonormalBasis.sum_inner_mul_inner v]
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simp_rw [OrthonormalBasis.sum_inner_mul_inner v]
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have {x : Fin (FiniteDimensional.finrank ℝ E)} : ∑ x_1 : Fin (FiniteDimensional.finrank ℝ E), ⟪v₁ x, v₁ x_1⟫_ℝ • v₁ x ⊗ₜ[ℝ] v₁ x_1 = v₁ x ⊗ₜ[ℝ] v₁ x := by
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have {i} : ∑ j, ⟪w i, w j⟫_ℝ • w i ⊗ₜ[ℝ] w j = w i ⊗ₜ[ℝ] w i := by
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rw [Fintype.sum_eq_single x, orthonormal_iff_ite.1 v₁.orthonormal]; simp
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rw [Fintype.sum_eq_single i, orthonormal_iff_ite.1 w.orthonormal]; simp
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intro r₁ hr₁
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intro _ _; rw [orthonormal_iff_ite.1 w.orthonormal]; simp; tauto
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rw [orthonormal_iff_ite.1 v₁.orthonormal]; simp; tauto
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simp_rw [this]
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simp_rw [this]
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rfl
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@ -10,7 +10,6 @@ import Mathlib.LinearAlgebra.Contraction
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open BigOperators
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open BigOperators
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open Finset
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open Finset
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lemma OrthonormalBasis.sum_repr'
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lemma OrthonormalBasis.sum_repr'
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{𝕜 : Type*} [RCLike 𝕜]
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{𝕜 : Type*} [RCLike 𝕜]
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{E : Type*} [NormedAddCommGroup E] [InnerProductSpace 𝕜 E]
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{E : Type*} [NormedAddCommGroup E] [InnerProductSpace 𝕜 E]
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@ -21,15 +20,53 @@ lemma OrthonormalBasis.sum_repr'
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nth_rw 1 [← (b.sum_repr v)]
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nth_rw 1 [← (b.sum_repr v)]
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simp_rw [b.repr_apply_apply v]
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simp_rw [b.repr_apply_apply v]
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variable {E : Type*} [NormedAddCommGroup E] [InnerProductSpace ℝ E] [FiniteDimensional ℝ E]
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noncomputable def realInnerAsElementOfDualTensorprod
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noncomputable def realInnerAsElementOfDualTensorprod
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{E : Type*} [NormedAddCommGroup E] [InnerProductSpace ℝ E]
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{E : Type*} [NormedAddCommGroup E] [InnerProductSpace ℝ E]
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: TensorProduct ℝ E E →ₗ[ℝ] ℝ := TensorProduct.lift bilinFormOfRealInner
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: TensorProduct ℝ E E →ₗ[ℝ] ℝ := TensorProduct.lift bilinFormOfRealInner
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instance
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{E : Type*} [NormedAddCommGroup E] [InnerProductSpace ℝ E] [CompleteSpace E] [FiniteDimensional ℝ E]
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: NormedAddCommGroup (TensorProduct ℝ E E) where
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norm := by
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sorry
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dist_self := by
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sorry
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sorry
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/-
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instance
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{E : Type*} [NormedAddCommGroup E] [InnerProductSpace ℝ E] [CompleteSpace E] [FiniteDimensional ℝ E]
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: InnerProductSpace ℝ (TensorProduct ℝ E E) where
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smul := _
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one_smul := _
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mul_smul := _
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smul_zero := _
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smul_add := _
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add_smul := _
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zero_smul := _
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norm_smul_le := _
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inner := _
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norm_sq_eq_inner := _
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conj_symm := _
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add_left := _
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smul_left := _
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-/
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noncomputable def dual'
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noncomputable def dual'
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{E : Type*} [NormedAddCommGroup E] [InnerProductSpace ℝ E] [CompleteSpace E] [FiniteDimensional ℝ E]
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{E : Type*} [NormedAddCommGroup E] [InnerProductSpace ℝ E] [CompleteSpace E] [FiniteDimensional ℝ E]
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: (TensorProduct ℝ E E →ₗ[ℝ] ℝ) ≃ₗ[ℝ] TensorProduct ℝ E E := by
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: (TensorProduct ℝ E E →ₗ[ℝ] ℝ) ≃ₗ[ℝ] TensorProduct ℝ E E := by
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let d := InnerProductSpace.toDual ℝ E
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let d := InnerProductSpace.toDual ℝ E
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let e := d.toLinearEquiv
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let e := d.toLinearEquiv
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let a := TensorProduct.congr e e
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let a := TensorProduct.congr e e
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