Imports
/-
Copyright (c) 2026 Joseph Tooby-Smith. All rights reserved.
Released under Apache 2.0 license as described in the file LICENSE.
Authors: Joseph Tooby-Smith
-/
module
public import Mathlib.Analysis.Complex.Basic
public import Physlib.Meta.TODO.Basic
public import Physlib.Relativity.SL2C.Basic
public import Physlib.Meta.Informal.Basic
public import Physlib.Meta.TODO.BasicRight handed Weyl fermions
In this file we define Right handed Weyl fermions.
These sit in the conjugate representation of SL(2,ℂ),
and we consider them to have up indices ψ^{\dot α} with α = 1,2.
@[expose] public section
The module in which right handed fermions live. This is equivalent to Fin 2 → ℂ.
The underlying value in Fin 2 → ℂ.
structure RightHandedWeyl where val : Fin 2 → ℂUnderlying module structure
The equivalence between RightHandedWeyl and Fin 2 → ℂ.
def toFin2ℂFun : RightHandedWeyl ≃ (Fin 2 → ℂ) where
toFun v := v.val
invFun f := ⟨f⟩
left_inv _ := rfl
right_inv _ := rfl
The instance of AddCommMonoid on RightHandedWeyl defined via its equivalence
with Fin 2 → ℂ.
instance : AddCommMonoid RightHandedWeyl := Equiv.addCommMonoid toFin2ℂFun
The instance of AddCommGroup on RightHandedWeyl defined via its equivalence
with Fin 2 → ℂ.
instance : AddCommGroup RightHandedWeyl := Equiv.addCommGroup toFin2ℂFun
The instance of Module on RightHandedWeyl defined via its equivalence
with Fin 2 → ℂ.
instance : Module ℂ RightHandedWeyl := Equiv.module ℂ toFin2ℂFun
The linear equivalence between RightHandedWeyl and (Fin 2 → ℂ).
@[simps!]
def toFin2ℂEquiv : RightHandedWeyl ≃ₗ[ℂ] (Fin 2 → ℂ) where
toFun := toFin2ℂFun
map_add' := fun _ _ => rfl
map_smul' := fun _ _ => rfl
invFun := toFin2ℂFun.symm
left_inv := fun _ => rfl
right_inv := fun _ => rfl
The underlying element of Fin 2 → ℂ of a element in RightHandedWeyl defined
through the linear equivalence toFin2ℂEquiv.
abbrev toFin2ℂ (ψ : RightHandedWeyl) := toFin2ℂEquiv ψlemma toFin2ℂ_eq_val (ψ : RightHandedWeyl) : ψ.toFin2ℂ = ψ.val := rflBasis
The standard basis on right-handed Weyl fermions.
def basis : Basis (Fin 2) ℂ RightHandedWeyl := Basis.ofEquivFun
(Equiv.linearEquiv ℂ RightHandedWeyl.toFin2ℂFun)lemma basis_apply (i j : Fin 2) : (basis i).1 j = if j = i then 1 else 0 := i:Fin 2j:Fin 2⊢ (basis i).val j = if j = i then 1 else 0
i:Fin 2j:Fin 2⊢ (toFin2ℂFun.symm (Pi.single i 1)).val j = if j = i then 1 else 0
i:Fin 2j:Fin 2⊢ Pi.single i 1 j = if j = i then 1 else 0
All goals completed! 🐙lemma eq_sum_basis (ψ : RightHandedWeyl) : ψ = ∑ i, ψ.1 i • basis i := ψ:RightHandedWeyl⊢ ψ = ∑ i, ψ.val i • basis i
conv_lhs => ψ:RightHandedWeyl| ∑ i, (basis.repr ψ) i • basis i
All goals completed! 🐙lemma basis_val (i : Fin 2) : (basis i).val = Pi.single i 1 := i:Fin 2⊢ (basis i).val = Pi.single i 1
i:Fin 2j:Fin 2⊢ (basis i).val j = Pi.single i 1 j
All goals completed! 🐙Representation
The vector space ℂ^2 carrying the conjugate representation of SL(2,C). In index notation corresponds to a Weyl fermion with indices ψ^{dot a}.
def rep : Representation ℂ SL(2,ℂ) RightHandedWeyl where
toFun := fun M => {
toFun := fun (ψ : RightHandedWeyl) =>
RightHandedWeyl.toFin2ℂEquiv.symm (M.1.map star *ᵥ ψ.toFin2ℂ),
map_add' := M:SL(2, ℂ)⊢ ∀ (x y : RightHandedWeyl),
toFin2ℂEquiv.symm ((↑M).map star *ᵥ (x + y).toFin2ℂ) =
toFin2ℂEquiv.symm ((↑M).map star *ᵥ x.toFin2ℂ) + toFin2ℂEquiv.symm ((↑M).map star *ᵥ y.toFin2ℂ)
M:SL(2, ℂ)ψ:RightHandedWeylψ':RightHandedWeyl⊢ toFin2ℂEquiv.symm ((↑M).map star *ᵥ (ψ + ψ').toFin2ℂ) =
toFin2ℂEquiv.symm ((↑M).map star *ᵥ ψ.toFin2ℂ) + toFin2ℂEquiv.symm ((↑M).map star *ᵥ ψ'.toFin2ℂ)
All goals completed! 🐙
map_smul' := M:SL(2, ℂ)⊢ ∀ (m : ℂ) (x : RightHandedWeyl),
toFin2ℂEquiv.symm ((↑M).map star *ᵥ (m • x).toFin2ℂ) =
(RingHom.id ℂ) m • toFin2ℂEquiv.symm ((↑M).map star *ᵥ x.toFin2ℂ)
M:SL(2, ℂ)r:ℂψ:RightHandedWeyl⊢ toFin2ℂEquiv.symm ((↑M).map star *ᵥ (r • ψ).toFin2ℂ) = (RingHom.id ℂ) r • toFin2ℂEquiv.symm ((↑M).map star *ᵥ ψ.toFin2ℂ)
All goals completed! 🐙}
map_one' := ⊢ { toFun := fun ψ => toFin2ℂEquiv.symm ((↑1).map star *ᵥ ψ.toFin2ℂ), map_add' := ⋯, map_smul' := ⋯ } = 1
i:RightHandedWeyl⊢ { toFun := fun ψ => toFin2ℂEquiv.symm ((↑1).map star *ᵥ ψ.toFin2ℂ), map_add' := ⋯, map_smul' := ⋯ } i = 1 i
All goals completed! 🐙
map_mul' := fun M N => M:SL(2, ℂ)N:SL(2, ℂ)⊢ { toFun := fun ψ => toFin2ℂEquiv.symm ((↑(M * N)).map star *ᵥ ψ.toFin2ℂ), map_add' := ⋯, map_smul' := ⋯ } =
{ toFun := fun ψ => toFin2ℂEquiv.symm ((↑M).map star *ᵥ ψ.toFin2ℂ), map_add' := ⋯, map_smul' := ⋯ } *
{ toFun := fun ψ => toFin2ℂEquiv.symm ((↑N).map star *ᵥ ψ.toFin2ℂ), map_add' := ⋯, map_smul' := ⋯ }
M:SL(2, ℂ)N:SL(2, ℂ)x:RightHandedWeyl⊢ { toFun := fun ψ => toFin2ℂEquiv.symm ((↑(M * N)).map star *ᵥ ψ.toFin2ℂ), map_add' := ⋯, map_smul' := ⋯ } x =
({ toFun := fun ψ => toFin2ℂEquiv.symm ((↑M).map star *ᵥ ψ.toFin2ℂ), map_add' := ⋯, map_smul' := ⋯ } *
{ toFun := fun ψ => toFin2ℂEquiv.symm ((↑N).map star *ᵥ ψ.toFin2ℂ), map_add' := ⋯, map_smul' := ⋯ })
x
All goals completed! 🐙lemma rep_apply (M : SL(2,ℂ)) (ψ : RightHandedWeyl) : rep M ψ = ⟨M.1.map star *ᵥ ψ.1⟩ := rflM:SL(2, ℂ)ψ:RightHandedWeyl⊢ ∑ i, ((rep M) ψ).val i • basis i = ∑ i, (∑ j, (↑M).map star i j * ψ.val j) • basis i
rfl All goals completed! 🐙
lemma rep_apply_basis (M : SL(2,ℂ)) (i : Fin 2) :
rep M (basis i) = ∑ j, M.1.map star j i • basis j := by M:SL(2, ℂ)i:Fin 2⊢ (rep M) (basis i) = ∑ j, (↑M).map star j i • basis j
rw [rep_apply_eq_sum_basis M:SL(2, ℂ)i:Fin 2⊢ ∑ i_1, (∑ j, (↑M).map star i_1 j * (basis i).val j) • basis i_1 = ∑ j, (↑M).map star j i • basis j M:SL(2, ℂ)i:Fin 2⊢ ∑ i_1, (∑ j, (↑M).map star i_1 j * (basis i).val j) • basis i_1 = ∑ j, (↑M).map star j i • basis j] M:SL(2, ℂ)i:Fin 2⊢ ∑ i_1, (∑ j, (↑M).map star i_1 j * (basis i).val j) • basis i_1 = ∑ j, (↑M).map star j i • basis j
congr e_f M:SL(2, ℂ)i:Fin 2⊢ (fun i_1 => (∑ j, (↑M).map star i_1 j * (basis i).val j) • basis i_1) = fun j => (↑M).map star j i • basis j
funext j e_f M:SL(2, ℂ)i:Fin 2j:Fin 2⊢ (∑ j_1, (↑M).map star j j_1 * (basis i).val j_1) • basis j = (↑M).map star j i • basis j
simp [basis_apply] All goals completed! 🐙
lemma rep_toMatrix (M : SL(2,ℂ)) : (LinearMap.toMatrix basis basis) (rep M) = M.1.map star := by M:SL(2, ℂ)⊢ (LinearMap.toMatrix basis basis) (rep M) = (↑M).map star
ext i j M:SL(2, ℂ)i:Fin 2j:Fin 2⊢ (LinearMap.toMatrix basis basis) (rep M) i j = (↑M).map star i j
rw [LinearMap.toMatrix_apply M:SL(2, ℂ)i:Fin 2j:Fin 2⊢ (basis.repr ((rep M) (basis j))) i = (↑M).map star i j M:SL(2, ℂ)i:Fin 2j:Fin 2⊢ (basis.repr ((rep M) (basis j))) i = (↑M).map star i j] M:SL(2, ℂ)i:Fin 2j:Fin 2⊢ (basis.repr ((rep M) (basis j))) i = (↑M).map star i j
simp only [basis, Basis.coe_ofEquivFun, Basis.ofEquivFun_repr_apply] M:SL(2, ℂ)i:Fin 2j:Fin 2⊢ (Equiv.linearEquiv ℂ toFin2ℂFun) ((rep M) ((Equiv.linearEquiv ℂ toFin2ℂFun).symm (Pi.single j 1))) i = (↑M).map star i j
change (M.1.map star *ᵥ (Pi.single j 1)) i = _ M:SL(2, ℂ)i:Fin 2j:Fin 2⊢ ((↑M).map star *ᵥ Pi.single j 1) i = (↑M).map star i j
simp All goals completed! 🐙lemma rep_apply_basis_repr (M : SL(2,ℂ)) (i j : Fin 2) :
basis.repr (rep M (basis i)) j = star (M.1 j i) := by M:SL(2, ℂ)i:Fin 2j:Fin 2⊢ (basis.repr ((rep M) (basis i))) j = star (↑M j i)
fin_cases j «0» M:SL(2, ℂ)i:Fin 2⊢ (basis.repr ((rep M) (basis i))) ((fun i => i) ⟨0, ⋯⟩) = star (↑M ((fun i => i) ⟨0, ⋯⟩) i)«1» M:SL(2, ℂ)i:Fin 2⊢ (basis.repr ((rep M) (basis i))) ((fun i => i) ⟨1, ⋯⟩) = star (↑M ((fun i => i) ⟨1, ⋯⟩) i) <;> «0» M:SL(2, ℂ)i:Fin 2⊢ (basis.repr ((rep M) (basis i))) ((fun i => i) ⟨0, ⋯⟩) = star (↑M ((fun i => i) ⟨0, ⋯⟩) i)«1» M:SL(2, ℂ)i:Fin 2⊢ (basis.repr ((rep M) (basis i))) ((fun i => i) ⟨1, ⋯⟩) = star (↑M ((fun i => i) ⟨1, ⋯⟩) i) simp [rep_apply_basis] All goals completed! 🐙