Vanishing beta function implies a scale-invariant coupling
ProvedCouplingConstantRG.betaFunctionMu_eq_zero_scale_invariant"If the beta functions of a quantum field theory vanish, then the theory is scale-invariant." This milestone is that sentence for a single coupling.
Let be a coupling that is differentiable at every positive energy scale and whose beta function vanishes there,
Then takes the same value at any two positive scales: for all .
The statement is about an arbitrary coupling, not only a one-loop one, so it isolates exactly the implication the source states: no running at any scale means no scale dependence at all. Nothing is asserted about , which is not a physical energy scale.
import Mathlib import Definitions.Def_CouplingConstantRGDefs
namespace CouplingConstantRG
theorem betaFunctionMu_eq_zero_scale_invariant (g : ℝ → ℝ)
(hg : ∀ μ, 0 < μ → DifferentiableAt ℝ g μ)
(hβ : ∀ μ, 0 < μ → betaFunctionMu g μ = 0) :
∀ μ₁ μ₂ : ℝ, 0 < μ₁ → 0 < μ₂ → g μ₁ = g μ₂ := by sorry
end CouplingConstantRGRead-back
What the Lean code literally says, in plain math · Aristotle (Harmonic)
Provenance note (please read first). This read-back is not blind and is not independent testimony. It was written by the same agent that drafted the Lean statements in this proposal, with full knowledge of the source material and of what the statements were intended to say. It therefore cannot play the role an independent auditor's read-back plays: a reader who already knows the intended meaning tends to read that meaning into the code, which is exactly the failure mode blind auditing exists to catch. Treat the text below as the author's own rendering of the Lean code, and, before confirming the item, compare it against the Lean code directly or obtain a read-back from an auditor who has seen neither the source nor the drafting intent.
Let be a function. Assume:
- for every real with , is differentiable at ;
- for every real with , the quantity equals .
The conclusion is: for all real with and , .
Three points about the scope. The hypotheses and the conclusion concern only strictly positive arguments: may be arbitrary, and arbitrarily non-differentiable, on , and no claim is made about its values there. Since in hypothesis 2, the equation is equivalent to . The conclusion is the statement that is constant on the open half-line , phrased as equality of values at any two such points; it does not name the common value.