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Explicit zero-temperature gap Δ(0)=ℏωD/sinh⁡(1/V0Z(EF))\Delta(0) = \hbar\omega_D / \sinh(1/V_0 Z(E_F))Δ(0)=ℏωD​/sinh(1/V0​Z(EF​))

Proved
BCSTheory.zeroTemperatureGap_eq

by Lucas · Oct 9, 2026 · Mathlib 0df444a (Lean v4.33.1)

bcs-theorysuperconductivity

Let ℏωD>0\hbar\omega_D>0ℏωD​>0 and λ=V0Z(EF)>0\lambda = V_0 Z(E_F) > 0λ=V0​Z(EF​)>0. A number Δ>0\Delta>0Δ>0 solves the zero-temperature gap equation 1λ=∫0ℏωDdηη2+Δ2\frac{1}{\lambda} = \int_0^{\hbar\omega_D} \frac{d\eta}{\sqrt{\eta^2+\Delta^2}}λ1​=∫0ℏωD​​η2+Δ2​dη​ if and only if Δ=ℏωD/sinh⁡(1/λ)\Delta = \hbar\omega_D/\sinh(1/\lambda)Δ=ℏωD​/sinh(1/λ); consequently Δ(0)=ℏωD/sinh⁡(1/λ)\Delta(0) = \hbar\omega_D/\sinh(1/\lambda)Δ(0)=ℏωD​/sinh(1/λ).

Preamble
import Mathlib
import Definitions.Def_BCSTheory_GapEquation
open Filter Topology
Formal statement
namespace BCSTheory

theorem zeroTemperatureGap_eq (hbarOmegaD coupling : ℝ) (hω : 0 < hbarOmegaD)
    (hc : 0 < coupling) :
    (∀ Δ : ℝ, 0 < Δ →
      (gapIntegralZeroTemp hbarOmegaD Δ = 1 / coupling ↔
        Δ = hbarOmegaD / Real.sinh (1 / coupling))) ∧
    zeroTemperatureGap hbarOmegaD coupling = hbarOmegaD / Real.sinh (1 / coupling) := by sorry

end BCSTheory
Source
Wikipedia (de), Artikel „BCS-Theorie“ (PDF-Ausdruck vom 05.10.2026), Abschnitt „Erfolge der BCS-Theorie“, Unterabschnitt „Existenz einer Energielücke“, zweite Formel; wiederholt im Unterabschnitt „Isotopeneffekt“.
Read-back

What the Lean code literally says, in plain math · Aristotle (Harmonic) — same agent as the drafter; non-blind

Non-blind read-back — not independent testimony. This read-back was written by the same agent (Aristotle, by Harmonic) that drafted the Lean statements, with full knowledge of the source text and of the intended meaning. It was not produced by a blind, independent auditor and must not be mistaken for independent testimony; an independent read-back is still advisable before launch.

Let ℏωD\hbar\omega_DℏωD​ and λ\lambdaλ be real numbers with ℏωD>0\hbar\omega_D>0ℏωD​>0 and λ>0\lambda>0λ>0. The statement asserts the conjunction of two claims:

  1. For every real Δ>0\Delta>0Δ>0:
∫0ℏωDdηη2+Δ2=1λ  ⟺  Δ=ℏωDsinh⁡(1/λ).\int_0^{\hbar\omega_D}\frac{d\eta}{\sqrt{\eta^2+\Delta^2}} = \frac1\lambda \iff \Delta = \frac{\hbar\omega_D}{\sinh(1/\lambda)}.∫0ℏωD​​η2+Δ2​dη​=λ1​⟺Δ=sinh(1/λ)ℏωD​​.
  1. The zero-temperature gap Δ0(ℏωD,λ)\Delta_0(\hbar\omega_D,\lambda)Δ0​(ℏωD​,λ), defined as the supremum of the set of all Δ>0\Delta>0Δ>0 satisfying the equation in (1) (with the convention sup⁡=0\sup = 0sup=0 for empty or unbounded sets), equals ℏωD/sinh⁡(1/λ)\hbar\omega_D/\sinh(1/\lambda)ℏωD​/sinh(1/λ).

Since λ>0\lambda>0λ>0, sinh⁡(1/λ)>0\sinh(1/\lambda)>0sinh(1/λ)>0, so the right-hand side is a positive number and no division by zero occurs.

Human review
  • Endorsed by Shuze Chen · Oct 10, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Lucas · Oct 10, 2026

    Confirmed by the mission captain (proposal self-audit).

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