2024-09-15 19:01:34 -04:00
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/-
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Copyright (c) 2024 Joseph Tooby-Smith. All rights reserved.
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Released under Apache 2.0 license as described in the file LICENSE.
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Authors: Joseph Tooby-Smith
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-/
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import HepLean.Meta.Informal
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2024-10-03 07:15:48 +00:00
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import HepLean.SpaceTime.SL2C.Basic
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import Mathlib.RepresentationTheory.Rep
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import HepLean.Tensors.Basic
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import HepLean.SpaceTime.WeylFermion.Modules
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import Mathlib.Logic.Equiv.TransferInstance
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2024-09-15 19:01:34 -04:00
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/-!
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# Weyl fermions
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2024-10-03 07:15:48 +00:00
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A good reference for the material in this file is:
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https://particle.physics.ucdavis.edu/modernsusy/slides/slideimages/spinorfeynrules.pdf
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2024-09-17 05:23:09 -04:00
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2024-09-15 19:01:34 -04:00
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-/
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2024-10-03 07:15:48 +00:00
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namespace Fermion
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noncomputable section
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open Matrix
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open MatrixGroups
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open Complex
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open TensorProduct
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/-- The vector space ℂ^2 carrying the fundamental representation of SL(2,C).
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2024-10-03 07:32:46 +00:00
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In index notation corresponds to a Weyl fermion with indices ψ_a. -/
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2024-10-03 07:15:48 +00:00
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def leftHanded : Rep ℂ SL(2,ℂ) := Rep.of {
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toFun := fun M => {
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toFun := fun (ψ : LeftHandedModule) =>
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LeftHandedModule.toFin2ℂEquiv.symm (M.1 *ᵥ ψ.toFin2ℂ),
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map_add' := by
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intro ψ ψ'
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simp [mulVec_add]
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map_smul' := by
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intro r ψ
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simp [mulVec_smul]}
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map_one' := by
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ext i
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simp
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map_mul' := fun M N => by
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simp only [SpecialLinearGroup.coe_mul]
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ext1 x
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simp only [LinearMap.coe_mk, AddHom.coe_mk, LinearMap.mul_apply, LinearEquiv.apply_symm_apply,
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mulVec_mulVec]}
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2024-10-15 11:29:18 +00:00
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/-- The standard basis on left-handed Weyl fermions. -/
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def leftBasis : Basis (Fin 2) ℂ leftHanded := Basis.ofEquivFun
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(Equiv.linearEquiv ℂ LeftHandedModule.toFin2ℂFun)
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@[simp]
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lemma leftBasis_ρ_apply (M : SL(2,ℂ)) (i j : Fin 2) :
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(LinearMap.toMatrix leftBasis leftBasis) (leftHanded.ρ M) i j = M.1 i j := by
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rw [LinearMap.toMatrix_apply]
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2024-10-15 11:53:24 +00:00
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simp only [leftBasis, Basis.coe_ofEquivFun, Basis.ofEquivFun_repr_apply]
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change (M.1 *ᵥ (Pi.single j 1)) i = _
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simp only [mulVec_single, mul_one]
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2024-10-03 07:15:48 +00:00
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/-- The vector space ℂ^2 carrying the representation of SL(2,C) given by
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2024-10-03 07:32:46 +00:00
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M → (M⁻¹)ᵀ. In index notation corresponds to a Weyl fermion with indices ψ^a. -/
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def altLeftHanded : Rep ℂ SL(2,ℂ) := Rep.of {
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toFun := fun M => {
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toFun := fun (ψ : AltLeftHandedModule) =>
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AltLeftHandedModule.toFin2ℂEquiv.symm ((M.1⁻¹)ᵀ *ᵥ ψ.toFin2ℂ),
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map_add' := by
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intro ψ ψ'
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simp [mulVec_add]
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map_smul' := by
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intro r ψ
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simp [mulVec_smul]}
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map_one' := by
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ext i
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simp
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map_mul' := fun M N => by
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ext1 x
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simp only [SpecialLinearGroup.coe_mul, LinearMap.coe_mk, AddHom.coe_mk, LinearMap.mul_apply,
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LinearEquiv.apply_symm_apply, mulVec_mulVec, EmbeddingLike.apply_eq_iff_eq]
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refine (congrFun (congrArg _ ?_) _)
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rw [Matrix.mul_inv_rev]
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exact transpose_mul _ _}
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2024-10-15 11:29:18 +00:00
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/-- The standard basis on alt-left-handed Weyl fermions. -/
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def altLeftBasis : Basis (Fin 2) ℂ altLeftHanded := Basis.ofEquivFun
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(Equiv.linearEquiv ℂ AltLeftHandedModule.toFin2ℂFun)
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@[simp]
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lemma altLeftBasis_ρ_apply (M : SL(2,ℂ)) (i j : Fin 2) :
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(LinearMap.toMatrix altLeftBasis altLeftBasis) (altLeftHanded.ρ M) i j = (M.1⁻¹)ᵀ i j := by
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rw [LinearMap.toMatrix_apply]
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simp only [altLeftBasis, Basis.coe_ofEquivFun, Basis.ofEquivFun_repr_apply, transpose_apply]
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change ((M.1⁻¹)ᵀ *ᵥ (Pi.single j 1)) i = _
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simp only [mulVec_single, transpose_apply, mul_one]
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2024-10-03 07:15:48 +00:00
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/-- The vector space ℂ^2 carrying the conjugate representation of SL(2,C).
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In index notation corresponds to a Weyl fermion with indices ψ_{dot a}. -/
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def rightHanded : Rep ℂ SL(2,ℂ) := Rep.of {
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toFun := fun M => {
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toFun := fun (ψ : RightHandedModule) =>
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RightHandedModule.toFin2ℂEquiv.symm (M.1.map star *ᵥ ψ.toFin2ℂ),
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map_add' := by
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intro ψ ψ'
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simp [mulVec_add]
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map_smul' := by
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intro r ψ
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simp [mulVec_smul]}
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map_one' := by
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ext i
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simp
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map_mul' := fun M N => by
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ext1 x
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simp only [SpecialLinearGroup.coe_mul, RCLike.star_def, Matrix.map_mul, LinearMap.coe_mk,
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AddHom.coe_mk, LinearMap.mul_apply, LinearEquiv.apply_symm_apply, mulVec_mulVec]}
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2024-10-15 11:29:18 +00:00
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/-- The standard basis on right-handed Weyl fermions. -/
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def rightBasis : Basis (Fin 2) ℂ rightHanded := Basis.ofEquivFun
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(Equiv.linearEquiv ℂ RightHandedModule.toFin2ℂFun)
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@[simp]
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lemma rightBasis_ρ_apply (M : SL(2,ℂ)) (i j : Fin 2) :
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(LinearMap.toMatrix rightBasis rightBasis) (rightHanded.ρ M) i j = (M.1.map star) i j := by
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rw [LinearMap.toMatrix_apply]
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simp only [rightBasis, Basis.coe_ofEquivFun, Basis.ofEquivFun_repr_apply, transpose_apply]
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change (M.1.map star *ᵥ (Pi.single j 1)) i = _
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simp only [mulVec_single, transpose_apply, mul_one]
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2024-10-03 07:15:48 +00:00
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/-- The vector space ℂ^2 carrying the representation of SL(2,C) given by
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M → (M⁻¹)^†.
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2024-10-03 07:32:46 +00:00
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In index notation this corresponds to a Weyl fermion with index `ψ^{dot a}`. -/
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2024-10-03 07:15:48 +00:00
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def altRightHanded : Rep ℂ SL(2,ℂ) := Rep.of {
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toFun := fun M => {
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toFun := fun (ψ : AltRightHandedModule) =>
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AltRightHandedModule.toFin2ℂEquiv.symm ((M.1⁻¹).conjTranspose *ᵥ ψ.toFin2ℂ),
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map_add' := by
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intro ψ ψ'
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simp [mulVec_add]
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map_smul' := by
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intro r ψ
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simp [mulVec_smul]}
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map_one' := by
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ext i
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simp
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map_mul' := fun M N => by
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ext1 x
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simp only [SpecialLinearGroup.coe_mul, LinearMap.coe_mk, AddHom.coe_mk, LinearMap.mul_apply,
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LinearEquiv.apply_symm_apply, mulVec_mulVec, EmbeddingLike.apply_eq_iff_eq]
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refine (congrFun (congrArg _ ?_) _)
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rw [Matrix.mul_inv_rev]
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exact conjTranspose_mul _ _}
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2024-10-15 11:29:18 +00:00
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/-- The standard basis on alt-right-handed Weyl fermions. -/
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def altRightBasis : Basis (Fin 2) ℂ altRightHanded := Basis.ofEquivFun
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(Equiv.linearEquiv ℂ AltRightHandedModule.toFin2ℂFun)
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@[simp]
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lemma altRightBasis_ρ_apply (M : SL(2,ℂ)) (i j : Fin 2) :
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(LinearMap.toMatrix altRightBasis altRightBasis) (altRightHanded.ρ M) i j =
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((M.1⁻¹).conjTranspose) i j := by
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rw [LinearMap.toMatrix_apply]
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simp only [altRightBasis, Basis.coe_ofEquivFun, Basis.ofEquivFun_repr_apply, transpose_apply]
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change ((M.1⁻¹).conjTranspose *ᵥ (Pi.single j 1)) i = _
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simp only [mulVec_single, transpose_apply, mul_one]
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2024-09-15 19:01:34 -04:00
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/-!
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## Equivalences between Weyl fermion vector spaces.
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-/
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2024-09-16 07:40:15 -04:00
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2024-10-03 07:15:48 +00:00
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/-- The morphism between the representation `leftHanded` and the representation
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`altLeftHanded` defined by multiplying an element of
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`leftHanded` by the matrix `εᵃ⁰ᵃ¹ = !![0, 1; -1, 0]]`. -/
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def leftHandedToAlt : leftHanded ⟶ altLeftHanded where
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hom := {
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toFun := fun ψ => AltLeftHandedModule.toFin2ℂEquiv.symm (!![0, 1; -1, 0] *ᵥ ψ.toFin2ℂ),
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map_add' := by
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intro ψ ψ'
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simp only [mulVec_add, LinearEquiv.map_add]
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map_smul' := by
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intro a ψ
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simp only [mulVec_smul, LinearEquiv.map_smul]
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rfl}
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comm := by
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intro M
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refine LinearMap.ext (fun ψ => ?_)
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change AltLeftHandedModule.toFin2ℂEquiv.symm (!![0, 1; -1, 0] *ᵥ M.1 *ᵥ ψ.val) =
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AltLeftHandedModule.toFin2ℂEquiv.symm ((M.1⁻¹)ᵀ *ᵥ !![0, 1; -1, 0] *ᵥ ψ.val)
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apply congrArg
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rw [mulVec_mulVec, mulVec_mulVec, SpaceTime.SL2C.inverse_coe, eta_fin_two M.1]
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refine congrFun (congrArg _ ?_) _
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rw [SpecialLinearGroup.coe_inv, Matrix.adjugate_fin_two,
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Matrix.mul_fin_two, eta_fin_two !![M.1 1 1, -M.1 0 1; -M.1 1 0, M.1 0 0]ᵀ]
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simp
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lemma leftHandedToAlt_hom_apply (ψ : leftHanded) :
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leftHandedToAlt.hom ψ =
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AltLeftHandedModule.toFin2ℂEquiv.symm (!![0, 1; -1, 0] *ᵥ ψ.toFin2ℂ) := rfl
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/-- The morphism from `altLeftHanded` to
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`leftHanded` defined by multiplying an element of
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altLeftHandedWeyl by the matrix `εₐ₁ₐ₂ = !![0, -1; 1, 0]`. -/
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def leftHandedAltTo : altLeftHanded ⟶ leftHanded where
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hom := {
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toFun := fun ψ =>
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LeftHandedModule.toFin2ℂEquiv.symm (!![0, -1; 1, 0] *ᵥ ψ.toFin2ℂ),
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map_add' := by
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intro ψ ψ'
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simp only [map_add]
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rw [mulVec_add, LinearEquiv.map_add]
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map_smul' := by
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intro a ψ
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simp only [LinearEquiv.map_smul]
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rw [mulVec_smul, LinearEquiv.map_smul]
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rfl}
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comm := by
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intro M
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refine LinearMap.ext (fun ψ => ?_)
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change LeftHandedModule.toFin2ℂEquiv.symm (!![0, -1; 1, 0] *ᵥ (M.1⁻¹)ᵀ *ᵥ ψ.val) =
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LeftHandedModule.toFin2ℂEquiv.symm (M.1 *ᵥ !![0, -1; 1, 0] *ᵥ ψ.val)
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rw [EquivLike.apply_eq_iff_eq, mulVec_mulVec, mulVec_mulVec, SpaceTime.SL2C.inverse_coe,
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eta_fin_two M.1]
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refine congrFun (congrArg _ ?_) _
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rw [SpecialLinearGroup.coe_inv, Matrix.adjugate_fin_two,
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Matrix.mul_fin_two, eta_fin_two !![M.1 1 1, -M.1 0 1; -M.1 1 0, M.1 0 0]ᵀ]
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simp
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lemma leftHandedAltTo_hom_apply (ψ : altLeftHanded) :
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leftHandedAltTo.hom ψ =
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LeftHandedModule.toFin2ℂEquiv.symm (!![0, -1; 1, 0] *ᵥ ψ.toFin2ℂ) := rfl
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/-- The equivalence between the representation `leftHanded` and the representation
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`altLeftHanded` defined by multiplying an element of
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`leftHanded` by the matrix `εᵃ⁰ᵃ¹ = !![0, 1; -1, 0]]`. -/
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def leftHandedAltEquiv : leftHanded ≅ altLeftHanded where
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hom := leftHandedToAlt
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inv := leftHandedAltTo
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hom_inv_id := by
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ext ψ
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simp only [Action.comp_hom, ModuleCat.coe_comp, Function.comp_apply, Action.id_hom,
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ModuleCat.id_apply]
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rw [leftHandedAltTo_hom_apply, leftHandedToAlt_hom_apply]
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rw [AltLeftHandedModule.toFin2ℂ, LinearEquiv.apply_symm_apply, mulVec_mulVec]
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rw [show (!![0, -1; (1 : ℂ), 0] * !![0, 1; -1, 0]) = 1 by simpa using Eq.symm one_fin_two]
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rw [one_mulVec]
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rfl
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inv_hom_id := by
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ext ψ
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simp only [Action.comp_hom, ModuleCat.coe_comp, Function.comp_apply, Action.id_hom,
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ModuleCat.id_apply]
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rw [leftHandedAltTo_hom_apply, leftHandedToAlt_hom_apply, LeftHandedModule.toFin2ℂ,
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LinearEquiv.apply_symm_apply, mulVec_mulVec]
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rw [show (!![0, (1 : ℂ); -1, 0] * !![0, -1; 1, 0]) = 1 by simpa using Eq.symm one_fin_two]
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rw [one_mulVec]
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rfl
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lemma leftHandedAltEquiv_hom_hom_apply (ψ : leftHanded) :
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leftHandedAltEquiv.hom.hom ψ =
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AltLeftHandedModule.toFin2ℂEquiv.symm (!![0, 1; -1, 0] *ᵥ ψ.toFin2ℂ) := rfl
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lemma leftHandedAltEquiv_inv_hom_apply (ψ : altLeftHanded) :
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leftHandedAltEquiv.inv.hom ψ =
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LeftHandedModule.toFin2ℂEquiv.symm (!![0, -1; 1, 0] *ᵥ ψ.toFin2ℂ) := rfl
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2024-09-15 19:01:34 -04:00
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2024-09-23 08:08:40 +00:00
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informal_definition rightHandedWeylAltEquiv where
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math :≈ "The linear equiv between rightHandedWeyl and altRightHandedWeyl given
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by multiplying an element of rightHandedWeyl by the matrix `εᵃ⁰ᵃ¹ = !![0, 1; -1, 0]]`"
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2024-10-03 07:15:48 +00:00
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deps :≈ [``rightHanded, ``altRightHanded]
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2024-09-15 19:01:34 -04:00
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2024-09-23 08:08:40 +00:00
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informal_lemma rightHandedWeylAltEquiv_equivariant where
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math :≈ "The linear equiv rightHandedWeylAltEquiv is equivariant with respect to the
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action of SL(2,C) on rightHandedWeyl and altRightHandedWeyl."
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deps :≈ [``rightHandedWeylAltEquiv]
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2024-09-16 13:41:52 -04:00
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2024-10-03 07:15:48 +00:00
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end
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2024-09-23 08:08:40 +00:00
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end Fermion
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