One-dimensional Lieb–Thirring conjecture

Let Lγ,1L_{\gamma,1} be the optimal Lieb–Thirring constant in dimension 11, and let Lγ,1clL_{\gamma,1}^{\mathrm{cl}} denote the semiclassical constant. Lieb–Thirring conjecture in dimension one. The optimal constant is

Lγ,1={2(γ1/2γ+1/2)γ1/2Lγ,1cl,1/2γ3/2,Lγ,1cl,3/2γ.L_{\gamma,1}=\begin{cases} 2\left(\frac{\gamma-1/2}{\gamma+1/2}\right)^{\gamma-1/2}L_{\gamma,1}^{\mathrm{cl}},&1/2\leq\gamma\leq3/2,\\ L_{\gamma,1}^{\mathrm{cl}},&3/2\leq\gamma. \end{cases}

This is the one-dimensional specialization of the Lieb–Thirring conjecture. It has been proved for γ=1/2\gamma=1/2 and for γ3/2\gamma\geq3/2, but remains open for 1/2<γ<3/21/2<\gamma<3/2.

Sources & referencesView supporting material

Primary source

Lukas Schimmer, “The state of the Lieb–Thirring conjecture”, arXiv:2203.06051 (2022).

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