Rakhmanov–Saff–Zhou logarithmic energy asymptotic conjecture for the sphere

Let Elog(S2;N)\mathcal{E}_{\mathrm{log}}(\mathbb{S}^2;N) denote the optimal logarithmic energy of NN points on the unit sphere, and let Clog,2C_{\mathrm{log},2} and Dlog,2D_{\mathrm{log},2} be constants independent of NN. Rakhmanov–Saff–Zhou's conjecture. There exist constants Clog,2C_{\mathrm{log},2} and Dlog,2D_{\mathrm{log},2} such that

Elog(S2;N)=(12log2)N212NlogN+Clog,2N+Dlog,2logN+O(1)as N.\mathcal{E}_{\mathrm{log}}(\mathbb{S}^2; N) = \left( \frac{1}{2} - \log 2 \right) N^2 - \frac{1}{2} N \log N + C_{\mathrm{log},2} \, N + D_{\mathrm{log},2} \, \log N + \mathcal{O}(1) \quad \text{as $N \to \infty$.}

This refines the known upper and lower bounds for the linear-order remainder in the logarithmic energy asymptotics.

Sources & referencesView supporting material

Primary source

J. S. Brauchart, D. P. Hardin and E. B. Saff, “The next-order term for optimal Riesz and logarithmic energy asymptotics on the sphere”, arXiv:1202.4037 (2012).

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