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With βh=0\beta_h=0βh​=0, the vacuum H=ϕ0=ϕ±=0H=\phi^0=\phi^\pm=0H=ϕ0=ϕ±=0 minimizes the potential

Proved
SMHiggsPotential.vacuum_minimizes_potential

by Lucas · Oct 1, 2026 · Mathlib 0df444a (Lean v4.33.1)

higgsparticle-physicsstandard-model

Let g,M,mhg,M,m_hg,M,mh​ be real and set βh=0\beta_h=0βh​=0. For all real H,ϕ0H,\phi^0H,ϕ0 and complex ϕ+\phi^+ϕ+,

LV(H,ϕ0,ϕ+)≤LV(0,0,0).\mathcal L_V(H,\phi^0,\phi^+)\le\mathcal L_V(0,0,0).LV​(H,ϕ0,ϕ+)≤LV​(0,0,0).

So the vacuum Φ=(0,v/2)\Phi=(0,v/\sqrt2)Φ=(0,v/2​) is a global minimum of the scalar potential V=−LVV=-\mathcal L_VV=−LV​ of box 2. (The degenerate cases M=0M=0M=0 or g=0g=0g=0 are included; there LV=−12mh2H2\mathcal L_V=-\frac12m_h^2H^2LV​=−21​mh2​H2 under the convention x/0=0x/0=0x/0=0.)

Preamble
import Mathlib
import Definitions.Def_SMHiggsPotential_Defs
open Complex
Formal statement
namespace SMHiggsPotential

theorem vacuum_minimizes_potential (g M mh H φ0 : ℝ) (φp : ℂ) :
    scalarLagrangian g M mh 0 H φ0 φp ≤ scalarLagrangian g M mh 0 0 0 0 := by sorry

end SMHiggsPotential
Source
Standard Model Lagrangian in Veltman's conventions (Feynman-'t Hooft gauge), as printed in the five-box chart supplied by the proposer (after M. Veltman, *Diagrammatica: The Path to Feynman Diagrams*, Cambridge University Press, 1994). Box 2, the non-derivative scalar terms: −12mh2H2-\frac12 m_h^2H^2−21​mh2​H2, the βh[… ]\beta_h[\dots]βh​[…] term, +2M4g2αh+\frac{2M^4}{g^2}\alpha_h+g22M4​αh​, −gα[H3+Hϕ0ϕ0+2Hϕ+ϕ−]-g\alpha[H^3+H\phi^0\phi^0+2H\phi^+\phi^-]−gα[H3+Hϕ0ϕ0+2Hϕ+ϕ−] and −18g2αh[H4+… ]-\frac18g^2\alpha_h[H^4+\dots]−81​g2αh​[H4+…].
Read-back

What the Lean code literally says, in plain math · Aristotle (Harmonic) - drafting agent, NON-BLIND (not an independent auditor)

NON-BLIND READ-BACK — NOT INDEPENDENT TESTIMONY. This read-back was written by the same agent (Aristotle, by Harmonic) that drafted the Lean statement, with full knowledge of the intended meaning and of the source image. It was not produced by a blind, independent auditor, and no reviewer should treat it as independent evidence that the formalization is faithful.

Binders. Real g,M,mh,H,ϕ0g,M,m_h,H,\phi^0g,M,mh​,H,ϕ0 and complex ϕ+\phi^+ϕ+; no hypotheses. The tadpole parameter is fixed to βh=0\beta_h=0βh​=0 on both sides.

Claim.

LV(g,M,mh,0;H,ϕ0,ϕ+)≤LV(g,M,mh,0;0,0,0).\mathcal L_V(g,M,m_h,0;H,\phi^0,\phi^+)\le\mathcal L_V(g,M,m_h,0;0,0,0).LV​(g,M,mh​,0;H,ϕ0,ϕ+)≤LV​(g,M,mh​,0;0,0,0).

This is a non-strict inequality, and M=0M=0M=0 or g=0g=0g=0 are allowed.

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