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 left handed Weyl fermions

In this file we define dual Left handed Weyl fermions. These sit in the dual of the fundamental representation of SL(2,ℂ), and we consider them to have down indices ψ_α with α = 1,2.

References

A good reference for the material in this file is: https://particle.physics.ucdavis.edu/modernsusy/slides/slideimages/spinorfeynrules.pdf Although a different index convention is used there.

@[expose] public section

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

The underlying value in Fin 2 → ℂ.

structure DualLeftHandedWeyl where val : Fin 2

Underlying module structure

The equivalence between DualLeftHandedWeyl and Fin 2 → ℂ.

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

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

instance : AddCommMonoid DualLeftHandedWeyl := Equiv.addCommMonoid toFin2ℂFun

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

instance : AddCommGroup DualLeftHandedWeyl := Equiv.addCommGroup toFin2ℂFun

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

instance : Module DualLeftHandedWeyl := Equiv.module toFin2ℂFun

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

@[simps!] def toFin2ℂEquiv : DualLeftHandedWeyl ≃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 DualLeftHandedWeyl defined through the linear equivalence toFin2ℂEquiv.

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

Basis

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

def basis : Basis (Fin 2) DualLeftHandedWeyl := Basis.ofEquivFun (Equiv.linearEquiv DualLeftHandedWeyl.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 : DualLeftHandedWeyl) : ψ = i, ψ.1 i basis i := ψ:DualLeftHandedWeylψ = i, ψ.val i basis i conv_lhs => ψ:DualLeftHandedWeyl| 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)ᵀ. In index notation corresponds to a left-handed Weyl fermion with indices ψ_a.

M:SL(2, )N:SL(2, )x:DualLeftHandedWeyl((↑N)⁻¹ * (↑M)⁻¹) = (↑M)⁻¹ * (↑N)⁻¹ All goals completed! 🐙
M:SL(2, )ψ:DualLeftHandedWeyl i, ((rep M) ψ).val i basis i = i, (∑ j, (↑M)⁻¹ j i * ψ.val j) basis i All goals completed! 🐙M:SL(2, )i:Fin 2 i_1, (∑ j, (↑M)⁻¹ j i_1 * (basis i).val j) basis i_1 = j, (↑M)⁻¹ i j basis j M:SL(2, )i:Fin 2(fun i_1 => (∑ j, (↑M)⁻¹ j i_1 * (basis i).val j) basis i_1) = fun j => (↑M)⁻¹ i j basis j M:SL(2, )i:Fin 2j:Fin 2(∑ j_1, (↑M)⁻¹ j_1 j * (basis i).val j_1) basis j = (↑M)⁻¹ i j 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 = M.1⁻¹ i j := M:SL(2, )i:Fin 2j:Fin 2(basis.repr ((rep M) (basis i))) j = (↑M)⁻¹ i j M:SL(2, )i:Fin 2(basis.repr ((rep M) (basis i))) ((fun i => i) 0, ) = (↑M)⁻¹ i ((fun i => i) 0, )M:SL(2, )i:Fin 2(basis.repr ((rep M) (basis i))) ((fun i => i) 1, ) = (↑M)⁻¹ i ((fun i => i) 1, ) M:SL(2, )i:Fin 2(basis.repr ((rep M) (basis i))) ((fun i => i) 0, ) = (↑M)⁻¹ i ((fun i => i) 0, )M:SL(2, )i:Fin 2(basis.repr ((rep M) (basis i))) ((fun i => i) 1, ) = (↑M)⁻¹ i ((fun i => i) 1, ) All goals completed! 🐙