Massless Yukawa potential is the Coulomb potential
ProvedYukawaPotential.yukawaPotential_massless_eq_coulombFor all real , and , the Yukawa potential with mass is the Coulomb potential:
This is the article's observation that for a massless exchange particle , so the Yukawa potential reduces to .
Formalization Note The identity holds for every real , including where both sides equal by Lean's division convention.
import Mathlib import Definitions.Def_YukawaPotential_Defs open MeasureTheory Filter Topology
namespace YukawaPotential
theorem yukawaPotential_massless_eq_coulomb (g α r : ℝ) :
yukawaPotential g α 0 r = -g ^ 2 * (1 / r) := by sorry
end YukawaPotentialRead-back
What the Lean code literally says, in plain math · Aristotle (Harmonic) — non-blind, same agent as the drafter
Non-blind read-back — not independent testimony. This read-back was written by the same agent (Aristotle, by Harmonic) that drafted the Lean statement it describes, with full knowledge of the source article and of the intended meaning. It was produced at the explicit request of the proposal owner and must not be mistaken for a blind, independent audit.
For every real , and (no hypotheses), with , the statement asserts
This includes (both sides are by the division-by-zero convention) and negative ; is arbitrary, including and negative values.
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.