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Sharp three-dimensional Lieb–Thirring constant

For scalar Schrödinger operators −Δ+V-\Delta+V on L2(R3)L^2(\mathbb R^3), is the optimal constant in Tr⁡(−Δ+V)−≤L1,3∫R3V−(x)5/2 dx\operatorname{Tr}(-\Delta+V)_-\le L_{1,3}\int_{\mathbb R^3}V_-(x)^{5/2}\,dx equal to its semiclassical value L1,3clL_{1,3}^{\mathrm{cl}}?

Source-reported statusAs of 2026-09-04Source & evidence ↓

Problem statement

For scalar Schrödinger operators −Δ+V-\Delta+V on L2(R3)L^2(\mathbb R^3), is the optimal constant in Tr⁡(−Δ+V)−≤L1,3∫R3V−(x)5/2 dx\operatorname{Tr}(-\Delta+V)_-\le L_{1,3}\int_{\mathbb R^3}V_-(x)^{5/2}\,dx equal to its semiclassical value L1,3clL_{1,3}^{\mathrm{cl}}?

Lean 4

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Background

Here V−=max⁡{−V,0}V_-=\max\{-V,0\}, and the trace is the sum of absolute values of negative eigenvalues. Fixing the kinetic-energy normalization and the first spectral moment makes this a concrete constant problem. It controls quantitative fermionic kinetic-energy inequalities and stability estimates.

Established baseline: general Lieb–Thirring inequalities and progressively improved bounds are available. The older conjecture giving a two-candidate formula for every dimension and exponent is partly disproved by Frank, Gontier and Lewin; it must not be advertised wholesale as open. The specified first-moment three-dimensional semiclassical equality is the retained target. Better certified upper bounds are useful partial progress, not a resolution.

Progress & source assessment

Source catalogue review: 4 September 2026. Improved indicates partial progress, including qualified preprint claims.

References
  1. [1]Frank, Gontier & Lewin, counterexamples to portions of the general Lieb–Thirring conjecture link
  2. [2]Frank, Hundertmark, Jex & Nam, improved Lieb–Thirring bounds link
  3. [3]Schimmer, review of Lieb–Thirring inequalities and surviving conjectures link

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