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Formalizations.Physics.Particles.GaugeHiggsUnification.NotchDecoupling

The notch decouples the fermion sector from the leading curvature #

The leading Kaluza–Klein order of the curvature at the half point is 𝒟 = π² (∑_{m ≡ 2 (4)} m² δ(m) − ∑_{m ≡ 0 (4)} m² δ(m)), with δ(m) = mult(m,0) − mult(m,1) over a finite set of levels. It is linear in δ and vanishes when δ(m) = 0 at every even m (the notch), so the fermion sector drops out and 𝒟 is the gauge part alone. On range (2N) it is the plain alternating weight −4π² ∑_{m' < N} (−1)^{m'} m'² δ(2m'). That 𝒟 is the leading curvature is physics and is not formalized here.

Main results #

References #

noncomputable def GaugeHiggsUnification.NotchDecoupling.curv (S : Finset ℕ) (δ : ℕ → ℝ) :

The leading Kaluza–Klein curvature built from the imbalance δ over the levels S.

Equations
Instances For
    theorem GaugeHiggsUnification.NotchDecoupling.curv_add (S : Finset ℕ) (δ₁ δ₂ : ℕ → ℝ) :
    curv S (δ₁ + δ₂) = curv S δ₁ + curv S δ₂
    theorem GaugeHiggsUnification.NotchDecoupling.curv_eq_zero_of_even {S : Finset ℕ} {δ : ℕ → ℝ} (h : ∀ m ∈ S, Even m → δ m = 0) :
    curv S δ = 0
    theorem GaugeHiggsUnification.NotchDecoupling.curv_decoupling {S : Finset ℕ} (δG δF : ℕ → ℝ) (h : ∀ m ∈ S, Even m → δF m = 0) :
    curv S (δG + δF) = curv S δG

    Decoupling: if the fermion imbalance vanishes on every even level, 𝒟 is the gauge part alone.

    theorem GaugeHiggsUnification.NotchDecoupling.curv_range_eq_alternating (N : ℕ) (δ : ℕ → ℝ) :
    curv (Finset.range (2 * N)) δ = -4 * Real.pi ^ 2 * ∑ k ∈ Finset.range N, (-1) ^ k * ↑k ^ 2 * δ (2 * k)

    The paper's rewriting m = 2m': a plain alternating weight.