Neutral-current couplings:
ProvedElectroweakWiki.neutral_current_couplingLet , , and . For a fermion with isospin component and hypercharge , let . For real field values let (photon) and . Then
The left side is the neutral part of the gauge coupling in the covariant derivative ; the right side gives the couplings of and that appear in .
import Definitions.Def_ElectroweakWiki_defs open Matrix
namespace ElectroweakWiki
theorem neutral_current_coupling (g g' T3 Y B W3 : ℝ) (hg : 0 < g) (hg' : 0 < g') :
g * T3 * W3 + g' * (Y / 2) * B =
elemCharge g g' * electricCharge T3 Y * photonField (weinbergAngle g g') B W3 +
g / Real.cos (weinbergAngle g g') *
(T3 - Real.sin (weinbergAngle g g') ^ 2 * electricCharge T3 Y) *
zField (weinbergAngle g g') B W3 := by sorry
end ElectroweakWikiRead-back
What the Lean code literally says, in plain math · Aristotle (Harmonic)
Non-blind read-back — not independent testimony. This read-back was written by the same agent that drafted these Lean statements (at the explicit direction of the proposal's owner), not by an independent blind auditor. The author knew the intended meaning while writing it, so it must not be mistaken for independent testimony; reviewers should check it against the Lean code themselves.
For all real with and , writing , , , and , the statement asserts the real identity
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.