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Eq. (4.4): ∑permi∫−∞0dη k12k22eiktη+c.c.=4∑i>jki2kj2kt\sum_{\rm perm}i\int_{-\infty}^0 d\eta\,k_1^2k_2^2e^{ik_t\eta}+{\rm c.c.} = 4\frac{\sum_{i>j}k_i^2k_j^2}{k_t}∑perm​i∫−∞0​dηk12​k22​eikt​η+c.c.=4kt​∑i>j​ki2​kj2​​

Proved
Maldacena2003.scalar_vertex_time_integral

by Lucas · Oct 12, 2026 · Mathlib 0df444a (Lean v4.33.1)

cosmologyinflationmathematical-physics

Let k1,k2,k3>0k_1,k_2,k_3>0k1​,k2​,k3​>0 and kt=k1+k2+k3k_t=k_1+k_2+k_3kt​=k1​+k2​+k3​. For ϵ>0\epsilon>0ϵ>0, put

S(ϵ)=∑σ∈S32 Re[ i∫−∞0kσ(1)2kσ(2)2 eiktη eϵη dη],S(\epsilon) = \sum_{\sigma\in S_3} 2\,\mathrm{Re}\Big[\, i\int_{-\infty}^{0} k_{\sigma(1)}^2k_{\sigma(2)}^2\, e^{ik_t\eta}\,e^{\epsilon\eta}\,d\eta\Big],S(ϵ)=σ∈S3​∑​2Re[i∫−∞0​kσ(1)2​kσ(2)2​eikt​ηeϵηdη],

the sum over the six permutations of the integral plus its complex conjugate. Then

lim⁡ϵ→0+S(ϵ)=4 k12k22+k12k32+k22k32kt.\lim_{\epsilon\to0^+} S(\epsilon) = 4\,\frac{k_1^2k_2^2+k_1^2k_3^2+k_2^2k_3^2}{k_t}.ϵ→0+lim​S(ϵ)=4kt​k12​k22​+k12​k32​+k22​k32​​.

This is the time integral in eq. (4.4). It gives the contribution of the cubic vertex of (3.11) to the three-scalar correlator in de Sitter space. The common prefactor (2π)3δ3(∑k⃗i)1∏(2ki3)ρ˙∗6ϕ˙∗2(2\pi)^3\delta^3(\sum\vec k_i)\frac{1}{\prod(2k_i^3)}\frac{\dot\rho_*^6}{\dot\phi_*^2}(2π)3δ3(∑ki​)∏(2ki3​)1​ϕ˙​∗2​ρ˙​∗6​​ of both sides is omitted.

Formalization Note The contour prescription η→η+iϵ∣η∣\eta\to\eta+i\epsilon|\eta|η→η+iϵ∣η∣ (the standard interacting vacuum) is implemented by the damping factor eϵηe^{\epsilon\eta}eϵη, followed by ϵ→0+\epsilon\to0^+ϵ→0+. The momenta are indexed by Fin 3, and the permutations are Equiv.Perm (Fin 3).

Preamble
import Mathlib
import Definitions.Def_Maldacena2003_InflationDefs
open Filter Topology
Formal statement
namespace Maldacena2003

theorem scalar_vertex_time_integral (k : Fin 3 → ℝ) (hk : ∀ i, 0 < k i) :
    Tendsto
      (fun ε : ℝ => ∑ σ : Equiv.Perm (Fin 3),
        2 * (Complex.I * ∫ η in Set.Iic (0 : ℝ),
          ((k (σ 0) : ℂ) ^ 2 * (k (σ 1) : ℂ) ^ 2)
            * Complex.exp (Complex.I * ((k 0 + k 1 + k 2 : ℝ) : ℂ) * (η : ℂ))
            * (Real.exp (ε * η) : ℂ)).re)
      (𝓝[>] 0)
      (𝓝 (4 * (k 1 ^ 2 * k 0 ^ 2 + k 2 ^ 2 * k 0 ^ 2 + k 2 ^ 2 * k 1 ^ 2)
        / (k 0 + k 1 + k 2))) := by sorry

end Maldacena2003
Source
J. Maldacena, Non-Gaussian features of primordial fluctuations in single field inflationary models, JHEP 05 (2003) 013, https://doi.org/10.1088/1126-6708/2003/05/013 (arXiv:astro-ph/0210603), p. 16, eq. (4.4)
Human review
  • Endorsed by Shuze Chen · Oct 13, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Lucas · Oct 13, 2026

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

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