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.Basic

Dual right handed Weyl fermions

In this file we define dual right handed Weyl fermions. These sit in the dual-conjugate representation of SL(2,ℂ), and we consider them to have down indices ψ_\dot α} with α = 1,2.

@[expose] public section

The module in which dual-right handed fermions live. This is equivalent to Fin 2 → ℂ.

The underlying value in Fin 2 → ℂ.

structure DualRightHandedWeyl where val : Fin 2

Underlying module structure

The equivalence between DualRightHandedWeyl and Fin 2 → ℂ.

def toFin2ℂFun : DualRightHandedWeyl (Fin 2 ) where toFun v := v.val invFun f := f left_inv _ := rfl right_inv _ := rfl

The instance of AddCommMonoid on DualRightHandedWeyl defined via its equivalence with Fin 2 → ℂ.

instance : AddCommMonoid DualRightHandedWeyl := Equiv.addCommMonoid toFin2ℂFun

The instance of AddCommGroup on DualRightHandedWeyl defined via its equivalence with Fin 2 → ℂ.

instance : AddCommGroup DualRightHandedWeyl := Equiv.addCommGroup toFin2ℂFun

The instance of Module on DualRightHandedWeyl defined via its equivalence with Fin 2 → ℂ.

instance : Module DualRightHandedWeyl := Equiv.module toFin2ℂFun

The linear equivalence between DualRightHandedWeyl and (Fin 2 → ℂ).

@[simps!] def toFin2ℂEquiv : DualRightHandedWeyl ≃ₗ[] (Fin 2 ) 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 DualRightHandedWeyl defined through the linear equivalence toFin2ℂEquiv.

abbrev toFin2ℂ (ψ : DualRightHandedWeyl) := toFin2ℂEquiv ψ
lemma toFin2ℂ_eq_val (ψ : DualRightHandedWeyl) : ψ.toFin2ℂ = ψ.val := rfl

Basis

The standard basis on dual-right-handed Weyl fermions.

def basis : Basis (Fin 2) DualRightHandedWeyl := Basis.ofEquivFun (Equiv.linearEquiv DualRightHandedWeyl.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 2Pi.single i 1 j = if j = i then 1 else 0 All goals completed! 🐙lemma eq_sum_basis (ψ : DualRightHandedWeyl) : ψ = i, ψ.1 i basis i := ψ:DualRightHandedWeylψ = i, ψ.val i basis i conv_lhs => ψ:DualRightHandedWeyl| 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 representation of SL(2,C) given by M → (M⁻¹)^†. In index notation this corresponds to a Weyl fermion with index ψ_{dot a}.

M:SL(2, )N:SL(2, )x:DualRightHandedWeyl((↑N)⁻¹ * (↑M)⁻¹) = (↑M)⁻¹ * (↑N)⁻¹ All goals completed! 🐙
lemma rep_apply (M : SL(2,)) (ψ : DualRightHandedWeyl) : rep M ψ = (M.1⁻¹).conjTranspose *ᵥ ψ.1 := rflM:SL(2, )ψ:DualRightHandedWeyl i, ((rep M) ψ).val i basis i = i, (∑ j, (↑M)⁻¹ i j * ψ.val j) basis i All goals completed! 🐙M:SL(2, )i:Fin 2 i_1, (∑ j, (↑M)⁻¹ i_1 j * (basis i).val j) basis i_1 = j, (↑M)⁻¹ j i basis j M:SL(2, )i:Fin 2(fun i_1 => (∑ j, (↑M)⁻¹ i_1 j * (basis i).val j) basis i_1) = fun j => (↑M)⁻¹ j i basis j M:SL(2, )i:Fin 2j:Fin 2(∑ j_1, (↑M)⁻¹ j j_1 * (basis i).val j_1) basis j = (↑M)⁻¹ j i basis j All goals completed! 🐙M:SL(2, )i:Fin 2j:Fin 2(basis.repr ((rep M) (basis j))) i = (↑M)⁻¹ i j M:SL(2, )i:Fin 2j:Fin 2(Equiv.linearEquiv toFin2ℂFun) ((rep M) ((Equiv.linearEquiv toFin2ℂFun).symm (Pi.single j 1))) i = (↑M)⁻¹ i j M:SL(2, )i:Fin 2j:Fin 2((↑M)⁻¹ *ᵥ Pi.single j 1) i = (↑M)⁻¹ i j All goals completed! 🐙lemma rep_apply_basis_repr (M : SL(2,)) (i j : Fin 2) : basis.repr (rep M (basis i)) j = star (M.1⁻¹ i j) := M:SL(2, )i:Fin 2j:Fin 2(basis.repr ((rep M) (basis i))) j = star ((↑M)⁻¹ i j) M:SL(2, )i:Fin 2(basis.repr ((rep M) (basis i))) ((fun i => i) 0, ) = star ((↑M)⁻¹ i ((fun i => i) 0, ))M:SL(2, )i:Fin 2(basis.repr ((rep M) (basis i))) ((fun i => i) 1, ) = star ((↑M)⁻¹ i ((fun i => i) 1, )) M:SL(2, )i:Fin 2(basis.repr ((rep M) (basis i))) ((fun i => i) 0, ) = star ((↑M)⁻¹ i ((fun i => i) 0, ))M:SL(2, )i:Fin 2(basis.repr ((rep M) (basis i))) ((fun i => i) 1, ) = star ((↑M)⁻¹ i ((fun i => i) 1, )) All goals completed! 🐙