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Yukawa potential as the inverse Fourier transform of −g2 4π/(k2+(αm)2)-g^2\,4\pi/(k^2+(\alpha m)^2)−g24π/(k2+(αm)2)

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YukawaPotential.yukawaPotential_inverse_fourier

by Lucas · Oct 3, 2026 · Mathlib 0df444a (Lean v4.33.1)

mathematical-physicsyukawa-potential

Let g∈Rg\in\mathbb Rg∈R, α>0\alpha>0α>0, m>0m>0m>0, and let x∈R3x\in\mathbb R^3x∈R3, x≠0x\neq0x=0. Then

V(∣x∣)=lim⁡Λ→∞  −g2(2π)3∫∣k∣<Λeik⋅x 4π∣k∣2+(αm)2 d3k,V(|x|) = \lim_{\Lambda\to\infty}\;\frac{-g^2}{(2\pi)^3}\int_{|k|<\Lambda} e^{i k\cdot x}\,\frac{4\pi}{|k|^2+(\alpha m)^2}\,d^3k,V(∣x∣)=Λ→∞lim​(2π)3−g2​∫∣k∣<Λ​eik⋅x∣k∣2+(αm)24π​d3k,

where V(r)=−g2e−αmr/rV(r)=-g^2e^{-\alpha m r}/rV(r)=−g2e−αmr/r and k⋅xk\cdot xk⋅x is the Euclidean inner product.

This is the formula of the section Fourier transform, with the integral over all momenta k∈R3k\in\mathbb R^3k∈R3 understood as the limit of integrals over balls.

Formalization Note The function 4π/(∣k∣2+(αm)2)4\pi/(|k|^2+(\alpha m)^2)4π/(∣k∣2+(αm)2) is not Lebesgue-integrable on R3\mathbb R^3R3, so the integral over all of R3\mathbb R^3R3 would be assigned the junk value 000 in Lean; the statement therefore takes the limit of the integrals over the open balls of radius Λ\LambdaΛ as Λ→∞\Lambda\to\inftyΛ→∞, computed in C\mathbb CC.

Preamble
import Mathlib
import Definitions.Def_YukawaPotential_Defs

open MeasureTheory Filter Topology
Formal statement
namespace YukawaPotential
theorem yukawaPotential_inverse_fourier (g α m : ℝ) (hα : 0 < α) (hm : 0 < m)
    (x : EuclideanSpace ℝ (Fin 3)) (hx : x ≠ 0) :
    Tendsto (fun Λ : ℝ => ((-g ^ 2 / (2 * Real.pi) ^ 3 : ℝ) : ℂ) *
        ∫ k in Metric.ball (0 : EuclideanSpace ℝ (Fin 3)) Λ,
          Complex.exp (Complex.I * (inner ℝ k x : ℝ)) *
            ((4 * Real.pi / (‖k‖ ^ 2 + (α * m) ^ 2) : ℝ) : ℂ))
      atTop (𝓝 ((yukawaPotential g α m ‖x‖ : ℝ) : ℂ)) := by sorry
end YukawaPotential
Source
Wikipedia, "Yukawa potential", revision oldid=1371658231, https://en.wikipedia.org/w/index.php?title=Yukawa_potential&oldid=1371658231, section 'Fourier transform': V(r) = (-g²/(2π)³) ∫ e^{ik·r} 4π/(k² + (αm)²) d³k.
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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.

Fix a real number ggg, real numbers α>0\alpha>0α>0 and m>0m>0m>0, and a point x∈R3x\in\mathbb R^3x∈R3 with x≠0x\neq0x=0. For each real Λ\LambdaΛ define the complex number

I(Λ)=−g2(2π)3∫{k∈R3: ∣k∣<Λ}ei ⟨k,x⟩ 4π∣k∣2+(αm)2 dk,I(\Lambda) = \frac{-g^2}{(2\pi)^3}\int_{\{k\in\mathbb R^3:\ |k|<\Lambda\}} e^{i\,\langle k,x\rangle}\,\frac{4\pi}{|k|^2+(\alpha m)^2}\,dk,I(Λ)=(2π)3−g2​∫{k∈R3: ∣k∣<Λ}​ei⟨k,x⟩∣k∣2+(αm)24π​dk,

a Bochner integral with respect to Lebesgue measure restricted to the open ball of radius Λ\LambdaΛ about the origin (empty, hence I(Λ)=0I(\Lambda)=0I(Λ)=0, when Λ≤0\Lambda\le0Λ≤0); ⟨k,x⟩\langle k,x\rangle⟨k,x⟩ is the Euclidean inner product and π\piπ is the circle constant. The statement asserts that I(Λ)I(\Lambda)I(Λ) converges in C\mathbb CC, as Λ→+∞\Lambda\to+\inftyΛ→+∞, to the real number −g2e−αm∣x∣/∣x∣-g^2 e^{-\alpha m|x|}/|x|−g2e−αm∣x∣/∣x∣ (viewed as a complex number).

Human review
  • Endorsed by Shuze Chen · Oct 8, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Lucas · Oct 8, 2026

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

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