The quartic bracket is
ProvedSMHiggsPotential.quartic_bracket_eq_sqhiggsparticle-physicsstandard-model
For all real (with in the application),
This is the bracket of the quartic term of box 2.
Preamble
import Mathlib import Definitions.Def_SMHiggsPotential_Defs open Complex
Formal statement
namespace SMHiggsPotential
theorem quartic_bracket_eq_sq (H φ0 p : ℝ) :
H ^ 4 + φ0 ^ 4 + 4 * p ^ 2 + 4 * φ0 ^ 2 * p + 4 * H ^ 2 * p + 2 * φ0 ^ 2 * H ^ 2 =
(H ^ 2 + φ0 ^ 2 + 2 * p) ^ 2 := by sorry
end SMHiggsPotentialSource
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: , the term, , and .
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. Three arbitrary real numbers ; no hypotheses ( may be negative).
Claim.