feat: Properties of 2HDM
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@ -4,6 +4,7 @@ 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.BeyondTheStandardModel.TwoHDM.Basic
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import HepLean.StandardModel.HiggsBoson.GaugeAction
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import Mathlib.LinearAlgebra.Matrix.PosDef
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/-!
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@ -22,38 +23,48 @@ open HiggsField
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noncomputable section
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/-- For two Higgs fields `Φ₁` and `Φ₂`, the map from space time to 2 x 2 complex matrices
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defined by ((Φ₁^†Φ₁, Φ₂^†Φ₁), (Φ₁^†Φ₂, Φ₂^†Φ₂)). -/
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defined by `((Φ₁^†Φ₁, Φ₂^†Φ₁), (Φ₁^†Φ₂, Φ₂^†Φ₂))`. -/
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def prodMatrix (Φ1 Φ2 : HiggsField) (x : SpaceTime) : Matrix (Fin 2) (Fin 2) ℂ :=
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!![⟪Φ1, Φ1⟫_H x, ⟪Φ2, Φ1⟫_H x; ⟪Φ1, Φ2⟫_H x, ⟪Φ2, Φ2⟫_H x]
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/-- The 2 x 2 complex matrices made up of components of the two Higgs fields. -/
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def fieldCompMatrix (Φ1 Φ2 : HiggsField) (x : SpaceTime) : Matrix (Fin 2) (Fin 2) ℂ :=
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!![Φ1 x 0, Φ1 x 1; Φ2 x 0, Φ2 x 1]
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/-- The matrix `prodMatrix Φ1 Φ2 x` is equal to the square of `fieldCompMatrix Φ1 Φ2 x`. -/
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lemma prodMatrix_eq_fieldCompMatrix_sq (Φ1 Φ2 : HiggsField) (x : SpaceTime) :
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prodMatrix Φ1 Φ2 x = fieldCompMatrix Φ1 Φ2 x * (fieldCompMatrix Φ1 Φ2 x).conjTranspose := by
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rw [fieldCompMatrix]
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trans !![Φ1 x 0, Φ1 x 1; Φ2 x 0, Φ2 x 1] *
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!![conj (Φ1 x 0), conj (Φ2 x 0); conj (Φ1 x 1), conj (Φ2 x 1)]
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· rw [Matrix.mul_fin_two, prodMatrix, innerProd_expand', innerProd_expand', innerProd_expand',
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innerProd_expand']
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funext i j
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fin_cases i <;> fin_cases j <;> ring_nf
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· funext i j
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fin_cases i <;> fin_cases j <;> rfl
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local instance : PartialOrder ℂ := Complex.partialOrder
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/-- The matrix `prodMatrix` is positive semi-definite. -/
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lemma prodMatrix_posSemiDef (Φ1 Φ2 : HiggsField) (x : SpaceTime) :
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(prodMatrix Φ1 Φ2 x).PosSemidef := by
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rw [Matrix.posSemidef_iff_eq_transpose_mul_self]
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use (fieldCompMatrix Φ1 Φ2 x).conjTranspose
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simpa using prodMatrix_eq_fieldCompMatrix_sq Φ1 Φ2 x
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/-- The matrix `prodMatrix` is hermitian. -/
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lemma prodMatrix_hermitian (Φ1 Φ2 : HiggsField) (x : SpaceTime) :
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(prodMatrix Φ1 Φ2 x).IsHermitian := by
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rw [Matrix.IsHermitian]
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ext i j
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fin_cases i <;> fin_cases j
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· simp [prodMatrix]
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· simp only [prodMatrix, innerProd, PiLp.inner_apply, RCLike.inner_apply, Fin.sum_univ_two,
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Fin.isValue, Fin.zero_eta, Fin.mk_one, Matrix.conjTranspose_apply, Matrix.of_apply,
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Matrix.cons_val', Matrix.cons_val_zero, Matrix.empty_val', Matrix.cons_val_fin_one,
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Matrix.cons_val_one, Matrix.head_fin_const, star_add, star_mul', RCLike.star_def,
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RingHomCompTriple.comp_apply, RingHom.id_apply, Matrix.head_cons]
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ring
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· simp only [prodMatrix, innerProd, PiLp.inner_apply, RCLike.inner_apply, Fin.sum_univ_two,
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Fin.isValue, Fin.mk_one, Fin.zero_eta, Matrix.conjTranspose_apply, Matrix.of_apply,
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Matrix.cons_val', Matrix.cons_val_one, Matrix.head_cons, Matrix.empty_val',
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Matrix.cons_val_fin_one, Matrix.cons_val_zero, star_add, star_mul', RCLike.star_def,
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RingHomCompTriple.comp_apply, RingHom.id_apply, Matrix.head_fin_const]
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ring
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· simp [prodMatrix]
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informal_lemma prodMatrix_positive_semidefinite where
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math :≈ "For all x in ``SpaceTime, ``prodMatrix at `x` is positive semidefinite."
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deps :≈ [``prodMatrix, ``SpaceTime]
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(prodMatrix Φ1 Φ2 x).IsHermitian := (prodMatrix_posSemiDef Φ1 Φ2 x).isHermitian
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informal_lemma prodMatrix_smooth where
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math :≈ "The map ``prodMatrix is a smooth function on spacetime."
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deps :≈ [``prodMatrix]
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informal_lemma prodMatrix_invariant where
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math :≈ "The map ``prodMatrix is invariant under the simultanous action of ``gaugeAction
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on the two Higgs fields."
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deps :≈ [``prodMatrix, ``gaugeAction]
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end
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end TwoHDM
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@ -66,6 +66,14 @@ lemma innerProd_right_zero (φ : HiggsField) : ⟪φ, 0⟫_H = 0 := by
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funext x
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simp [innerProd]
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/-- Expands the inner product on Higgs fields in terms of complex components of the
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Higgs fields. -/
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lemma innerProd_expand' (φ1 φ2 : HiggsField) (x : SpaceTime) :
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⟪φ1, φ2⟫_H x = conj (φ1 x 0) * φ2 x 0 + conj (φ1 x 1) * φ2 x 1 := by
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simp [innerProd]
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/-- Expands the inner product on Higgs fields in terms of real components of the
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Higgs fields. -/
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lemma innerProd_expand (φ1 φ2 : HiggsField) :
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⟪φ1, φ2⟫_H = fun x => equivRealProdCLM.symm (((φ1 x 0).re * (φ2 x 0).re
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+ (φ1 x 1).re * (φ2 x 1).re+ (φ1 x 0).im * (φ2 x 0).im + (φ1 x 1).im * (φ2 x 1).im),
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