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A Coulomb ground-state density without Kohn-Sham ensemble representation
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Abstract
We construct a finite three-electron Coulomb molecule whose spin-summed ground-state density cannot be reproduced by any ground-state ensemble of noninteracting electrons in a single real, spin-independent local potential in $L^{3/2}(\mathbf R^3)+L^\infty(\mathbf R^3)$. The molecule has two equal positive integer nuclear charges, specified by an exact finite nonnumerical formula.
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Collected automatically by AI tools (Claude Opus 5.5 and GPT-6 Astra, 2026-10-21) and not checked by a person. May be wrong or incomplete. Report an error.
Follow-up works
- Cody Haycraft, A Kohn–Sham Hamiltonian for the OpenAI three-electron density: a note on representability beyond L^{3/2}+L^∞ (GitHub working draft, status updated 2026-10-10). A response note that keeps the paper's exclusion in L^{3/2}+L^∞ and argues that a Friedrichs realisation of the candidate potential V = Δg/(2g) gives a Kohn–Sham Hamiltonian with ground-state density n (Theorem A). Per its README, a further theorem depends on an open estimate (Estimate 5.5), and the auxiliary Lean lemmas do not verify the analytic content.
Comments and discussion
- r/comp_chem participants, OpenAI paper on Kohn-Sham DFT (Reddit discussion, accessed 2026-10-21). Community participants discuss the construction's scale and the distinction between density-functional theory and noninteracting representability, and link earlier literature; their specialist credentials are not established in the thread.
Related prior literature mentioned by others
- Arno Schindlmayr and R. W. Godby, Density-functional theory and the v-representability problem for model strongly correlated electron systems (arXiv:cond-mat/9709266, 1997-09-24). Linked in the r/comp_chem discussion as background on noninteracting representability; it studies Hubbard-type systems with occupation and orbital-overlap density variables, a different setting from the paper's continuum Coulomb molecule.
Possibly relevant literature (found by the agent, not checked)
- H. Englisch and R. Englisch, Hohenberg-Kohn theorem and non-V-representable densities (Physica A 121 (1983) 253–268, doi:10.1016/0378-4371(83)90254-6). Gives early examples of densities that are not ensemble-V-representable, bearing on the paper's discussion of prescribed densities that fail representability (Section 1.1), where the paper cites only Wagner et al.
- P. E. Lammert, Differentiability of Lieb functional in electronic density functional theory (Int. J. Quantum Chem. 107 (2007) 1943–1953). Analyses when directional derivatives of the Lieb functional are given by a potential, relevant to the paper's corollary excluding a local-potential first variation of the ensemble Hxc functional.
- Nan Sheng, Exact density-functional theory as parallel ensemble variational hierarchies: from Lieb's formulation to Kohn-Sham theory (arXiv:2603.23399, revised 2026-07-23). Distinguishes constrained-search feasibility from attainment by a representing potential, which is background for the paper's ensemble-representability obstruction and its consequence for local-potential first variations.
- S. Kvaal, U. Ekström, A. M. Teale, T. Helgaker, Differentiable but exact formulation of density-functional theory (arXiv:1312.3734, 2013; doi:10.1063/1.4867005). A Moreau–Yosida regularised Kohn–Sham formulation that avoids the noninteracting representability problem in a finite box, giving context for the scope of the paper's non-representability and first-variation statements.
- T. C. Corso, v-representability and Hohenberg-Kohn theorem for non-interacting Schrödinger operators with distributional potentials in the one-dimensional torus (arXiv:2501.13513, 2025). A positive noninteracting v-representability result on the 1D torus with distributional potentials, complementing the existence results the paper contrasts with its own (Sutter et al.; Corso's 1D interval paper).
Elsewhere
- VibeMathed: Problem record
- Emergent Mind: family 278
Independent sites; their content is not reviewed here.
Cite
@misc{OAI:A-Coulomb-Ground-State-Density-without-Kohn-Sham-Ensemble-Representation-September-25-2026,
author = {{OpenAI}},
title = {{A Coulomb ground-state density without Kohn--Sham ensemble representation}},
howpublished = {OpenAI Math Release preprint
\href{https://github.com/openai/math/blob/main/preprints/A-Coulomb-Ground-State-Density-without-Kohn-Sham-Ensemble-Representation-September-25-2026/paper.pdf}{OAI:A-Coulomb-Ground-State-Density-without-Kohn-Sham-Ensemble-Representation-September-25-2026}},
year = {2026}
}Family 278: Failure of Kohn–Sham ensemble representation
Constructs a three-electron Coulomb molecule with two equal positive-integer-charge nuclei whose absolute ground-state density has no noninteracting ground-state ensemble representation by a single real spin-independent local potential in $L^{3/2}(\mathbb R^3)+L^\infty(\mathbb R^3)$. This disproves Kohn–Sham ensemble representability for that potential class; the required nuclear charge is specified nonnumerically.
This is the only paper in this family.