analysis / Discrete energy on the sphere; asymptotics of optimal logarithmic energy

The Brauchart-Hardin-Saff conjecture on the linear term of optimal logarithmic energy on the 2-sphere

Corollary 1.3: Elog⁡(n)=(12−log⁡2)n2−n2log⁡n+CBHSn+o(n)E_{\log}(n)=(\tfrac12-\log2)n^2-\tfrac n2\log n+C_{\mathrm{BHS}}n+o(n) with the Brauchart-Hardin-Saff constant, obtained from the triangular minimality of the planar Coulomb renormalized energy and the Betermin-Sandier equivalence. It is the logarithmic, d=2d=2 case only; the Riesz-energy cases of the Brauchart-Hardin-Saff conjectures and higher spheres are not addressed, and no explicit point configurations are produced.

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analysisSep 23, 2026Significance 30/100Registry: unreviewed

The Brauchart-Hardin-Saff conjecture on the linear term of optimal logarithmic energy on the 2-sphere

Prior state unknown→proved

Corollary 1.3: Elog⁡(n)=(12−log⁡2)n2−n2log⁡n+CBHSn+o(n)E_{\log}(n)=(\tfrac12-\log2)n^2-\tfrac n2\log n+C_{\mathrm{BHS}}n+o(n) with the Brauchart-Hardin-Saff constant, obtained from the triangular minimality of the planar Coulomb renormalized energy and the Betermin-Sandier equivalence. It is the logarithmic, d=2d=2 case only; the Riesz-energy cases of the Brauchart-Hardin-Saff conjectures and higher spheres are not addressed, and no explicit point config…

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Corollary 1.3: Elog⁡(n)=(12−log⁡2)n2−n2log⁡n+CBHSn+o(n)E_{\log}(n)=(\tfrac12-\log2)n^2-\tfrac n2\log n+C_{\mathrm{BHS}}n+o(n) with the Brauchart-Hardin-Saff constant, obtained from the triangular minimality of the planar Coulomb renormalized energy and the Betermin-Sandier equivalence. It is the logarithmic, d=2d=2 case only; the Riesz-energy cases of the Brauchart-Hardin-Saff conjectures and higher spheres are not addressed, and no explicit point configurations are produced.

Corollary 1.3: Elog⁡(n)=(12−log⁡2)n2−n2log⁡n+CBHSn+o(n)E_{\log}(n)=(\tfrac12-\log2)n^2-\tfrac n2\log n+C_{\mathrm{BHS}}n+o(n) with the Brauchart-Hardin-Saff constant, obtained from the triangular minimality of the planar Coulomb renormalized energy and the Betermin-Sandier equivalence. It is the logarithmic, d=2d=2 case only; the Riesz-energy cases of the Brauchart-Hardin-Saff conjectures and higher spheres are not addressed, and no explicit point configurations are produced.

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The Brauchart-Hardin-Saff conjecture on the linear term of optimal logarithmic energy on the 2-sphere — Mathematical Frontier Network