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Thomson N=7N=7N=7: cubic lower bound for the energy excess over the pentagonal bipyramid

Proved
ThomsonN7.Reg.energy_ge_cubic

by Lucas · Oct 10, 2026 · Mathlib 0df444a (Lean v4.33.1)

discrete-geometrythomson-problem

Let P=(P0,…,P6)P=(P_0,\dots,P_6)P=(P0​,…,P6​) be the pentagonal bipyramid with the regular pentagon Pk=(cos⁡2πk5,sin⁡2πk5,0)P_k=(\cos\tfrac{2\pi k}5,\sin\tfrac{2\pi k}5,0)Pk​=(cos52πk​,sin52πk​,0) at indices k=0,…,4k=0,\dots,4k=0,…,4 and the poles (0,0,±1)(0,0,\pm1)(0,0,±1) at indices 5,65,65,6; let φ(t)=(2−2t)−1/2\varphi(t)=(2-2t)^{-1/2}φ(t)=(2−2t)−1/2, so that ∥x−y∥−1=φ(⟨x,y⟩)\|x-y\|^{-1}=\varphi(\langle x,y\rangle)∥x−y∥−1=φ(⟨x,y⟩) for unit vectors, and write gij=⟨Pi,Pj⟩g_{ij}=\langle P_i,P_j\ranglegij​=⟨Pi​,Pj​⟩ and E(y)=∑i<j∥yi−yj∥−1E(y)=\sum_{i<j}\|y_i-y_j\|^{-1}E(y)=∑i<j​∥yi​−yj​∥−1. Let Wij=φ(gij)3W_{ij}=\varphi(g_{ij})^3Wij​=φ(gij​)3 for i≠ji\ne ji=j, Wii=0W_{ii}=0Wii​=0, and μi=∑jWijgij\mu_i=\sum_j W_{ij}g_{ij}μi​=∑j​Wij​gij​.

Let y=(y0,…,y6)y=(y_0,\dots,y_6)y=(y0​,…,y6​) be seven pairwise distinct unit vectors in R3\mathbb R^3R3, write hi=yi−Pih_i=y_i-P_ihi​=yi​−Pi​ and τij=⟨yi,yj⟩−gij\tau_{ij}=\langle y_i,y_j\rangle-g_{ij}τij​=⟨yi​,yj​⟩−gij​. Then

12∑i,jWij⟨hi,hj⟩−12∑iμi∥hi∥2+∑i<j(32φ(gij)5τij2+52φ(gij)7τij3) ≤ E(y)−E(P).\tfrac12\sum_{i,j}W_{ij}\langle h_i,h_j\rangle-\tfrac12\sum_i\mu_i\|h_i\|^2+\sum_{i<j}\Big(\tfrac32\varphi(g_{ij})^5\tau_{ij}^2+\tfrac52\varphi(g_{ij})^7\tau_{ij}^3\Big)\ \le\ E(y)-E(P).21​i,j∑​Wij​⟨hi​,hj​⟩−21​i∑​μi​∥hi​∥2+i<j∑​(23​φ(gij​)5τij2​+25​φ(gij​)7τij3​) ≤ E(y)−E(P).

It follows from the pairwise Taylor/Bregman bound φ(g+τ)≥φ(g)+φ′(g)τ+12φ′′(g)τ2+16φ′′′(g)τ3\varphi(g+\tau)\ge\varphi(g)+\varphi'(g)\tau+\tfrac12\varphi''(g)\tau^2+\tfrac16\varphi'''(g)\tau^3φ(g+τ)≥φ(g)+φ′(g)τ+21​φ′′(g)τ2+61​φ′′′(g)τ3 on [−1,1)[-1,1)[−1,1) together with the first-order (equilibrium) identity of PPP, which rewrites the linear terms as the WWW/μ\muμ quadratic form.

Formalization Note All named objects (pentBipyramid, coulombEnergy, Base.phi, Reg.W, Reg.muP, Reg.gP, Reg.tau, Reg.Dpair, Reg.Qhess, Reg.Pen, Glue.TubeRigid) come from the platform definition ThomsonN7_core, taken verbatim from the source; R3 is EuclideanSpace ℝ (Fin 3).

Preamble
import Definitions.Def_ThomsonN7_core
Formal statement
namespace ThomsonN7

theorem Reg.energy_ge_cubic {y : Fin 7 → R3} (hy : ∀ i, ‖y i‖ = 1) (hinj : Function.Injective y) :
    1 / 2 * ∑ i, ∑ j, Reg.W i j * inner ℝ (y i - pentBipyramid i) (y j - pentBipyramid j)
      - 1 / 2 * ∑ i, Reg.muP i * ‖y i - pentBipyramid i‖ ^ 2
      + ∑ i, ∑ j ∈ Finset.Ioi i, (3 / 2 * Base.phi (Reg.gP i j) ^ 5 * Reg.tau y i j ^ 2
          + 5 / 2 * Base.phi (Reg.gP i j) ^ 7 * Reg.tau y i j ^ 3)
      ≤ coulombEnergy y - coulombEnergy pentBipyramid := by sorry

end ThomsonN7
Source
H. Tran, Thomson problem N = 7 Lean proof package, https://github.com/huwngtran/thomson-n7-lean @ 25f2fa53119273458cfbb3c4230904bffdd61e53: paper/PAPER.md §7.2 step 5 (local minimality); Lean `ThomsonN7.Reg.energy_ge_cubic`, https://github.com/huwngtran/thomson-n7-lean/blob/25f2fa53119273458cfbb3c4230904bffdd61e53/formal/lean/ThomsonN7/Solution.lean#L6703

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