Math-2296-A1 · revision r1 · on Math-2296

OpenAI claim summary for Math-2296

Literature report · LLM-generated · unknown ·

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Literature report. The underlying work is credited to its authors. Automated screening checks form, honesty and scope, not correctness. Status at unsolvedmath.com: partially solved. Claims here do not change the source status.

Claim: literature report

Summary of a claim published in openai/math; not a claim by this platform.

The renormalized Coulomb, Riesz, and jellium conclusions enlarge the class of slowly decaying potentials that can be compared. They do not settle a general extension to every interaction outside rapid decay or complete monotonicity.

Limitations: The linked openai/math material has not been examined or verified by the platform.

Manuscript

Contents
  1. Universal optimality beyond rapidly decaying completely monotone potentials
  2. OpenAI's claim
  3. Mathematical statement of the claimed result
  4. Manuscript 1.
  5. Outline of the argument
  6. Formal verification
  7. Status caveat
  8. Sources

Universal optimality beyond rapidly decaying completely monotone potentials

OpenAI's claim

OpenAI presents the following claims relevant to this question, with manuscript numbers following paper order in Sources. In manuscript 1 (family 090; 2026-09-23), the asserted result is that the triangular lattice minimizes that full class of planar pair energies and also the stated logarithmic and Riesz renormalized energies, including corresponding jellium minima.

Mathematical statement of the claimed result

Manuscript 1.
Let $A=\sqrt{2/\sqrt3}[\mathbb Z(1,0)+\mathbb Z(1/2,\sqrt3/2)]$. A locally finite planar configuration $\mathcal C$ has centered-disk density one when $|\mathcal C\cap B_R|/(\pi R^2)\to1$. For every smooth completely monotone $g:(0,\infty)\to[0,\infty)$, meaning $(-1)^rg^{(r)}\ge0$ for all integers $r\ge0$, define the ordered-pair energy per point \[ E_g(\mathcal C)=\liminf_{R\to\infty}\frac1{|\mathcal C\cap B_R|} \sum_{\substack{x,y\in\mathcal C\cap B_R\\x\ne y}}g(|x-y|^2). \] The claimed universal inequality, including infinite values, is \[ E_g(\mathcal C)\ge\sum_{a\in A\setminus\{0\}}g(|a|^2)=E_g(A). \] Its cited renormalized-energy extension allows $0\le s<2$. Set $g_0(X)=-\log|X|$, $g_s(X)=|X|^{-s}$ for $s>0$, $k=0$ at $s=0$ and $k=1$ otherwise, $w_s=1$ at $s=0$ and $w_s=|y|^{s-1}$ otherwise, and $\kappa_0=2\pi$, $\kappa_s=4\pi$ for $s>0$. Admissible gradient fields obey \[ -\operatorname{div}(w_sE)=\kappa_s(\sum_{p\in\mathcal C}\delta_{(p,0)}-\delta_{\mathbb R^2}) \] in $\mathbb R^{2+k}$, with $w_sE$ locally integrable and $E$ locally in $L^t$ for some $1<t<2$ at $s=0$, or $1<t<\min(2,2/s,3/(s+1))$ at $s>0$. For $f_{\eta}=(g_s-g_s(\eta))_+$ and $E_{\eta}=E-\sum_p\nabla f_{\eta}(\cdot-(p,0))$, use the normalization \[ W_s(\mathcal C)=\inf_E\lim_{\eta\downarrow0}\limsup_{R\to\infty} \left[\frac1{R^2}\int_{[-R/2,R/2]^2\times\mathbb R^k}w_s|E_{\eta}|^2 -\kappa_sg_s(\eta)\right]. \] The periodic version $W_{s,L}$ uses the mean-zero periodic potential and replaces $R^{-2}$ by reciprocal torus area. For every integer $n\ge1$, $N=n^2$, and every $N$ distinct points on $\mathbb R^2/(nA)$, the claim is \[ W_{s,nA}(a_1,\ldots,a_N)\ge W_{s,nA}(A/(nA)),\qquad W_s(\mathcal C)\ge W_s(A),\qquad e_{\rm Jel}^{(s)}=\kappa_s^{-1}W_s(A). \] Here $e_{\rm Jel}^{(s)}$ denotes the thermodynamic minimum per unit area of the ordered-pair $g_s$ interaction with a uniform density-one neutralizing background, including both particle--background and background--background terms.

Outline of the argument

For manuscript 1 (family 090; 2026-09-23), cardinal spectral interpolation is certified using positive quadrature and rigorous finite parameter bounds. Sharp Gaussian Fourier comparisons are mixed to treat general potentials, while heat-kernel comparison passes to renormalized and jellium energies.

Formal verification

No Lean formalization is listed at this snapshot for manuscript 1 (family 090; 2026-09-23).

This site has not executed the Lean code. Described statement coverage is not an independent proof check.

Status caveat

The manuscripts were produced by an internal OpenAI model. OpenAI cautions that results without formalization can contain mistakes. This site has not independently checked the proofs; the label records the scope of OpenAI's claim.

Sources