Gontier–Lewin–Nazar's finite-rank optimizer conjecture

Let d2d\geq 2, let q>1q>1, and let γ\gamma be a density matrix satisfying 0γ10\leq\gamma\leq 1. Write

γ=n=1Nunun\gamma=\sum_{n=1}^N |u_n\rangle\langle u_n|

for a rank-NN projection, and let ργ\rho_\gamma denote its density. The associated ground-state equations are

(Δργq1)un=μnun,(-\Delta-\rho_\gamma^{q-1})u_n=-\mu_nu_n,

where μ1<μ2<μN0-\mu_1< -\mu_2<\cdots\leq -\mu_N\leq 0 are the NN lowest eigenvalues of Δργq1-\Delta-\rho_\gamma^{q-1} on L2(Rd)L^2(\mathbb{R}^d). Optimizers of Lieb--Thirring interpolation inequalities. In the mass-subcritical case q<1+2/dq<1+2/d, for every N2N\geq 2 there exists a ground-state solution of rank NN; in the mass-supercritical case q>1+2/dq>1+2/d, there exists a finite integer N0N_0 such that no ground state of rank NN exists for N>N0N>N_0. In particular, there exists a global optimizer of finite rank. The conjecture formulates a sharp dichotomy between the mass-subcritical and mass-supercritical regimes. The subcritical assertion was previously proved only for qq sufficiently close to 11, with partial results across the full range, while the stated supercritical finite-rank conclusion remained open in the source.

Sources & referencesView supporting material

Primary source

Giao Ky Duong, Thi Minh Thao Le, Phan Thành Nam and Phuoc-Tai Nguyen, “Finite-Rank Optimizers for the mass–supercritical Lieb–Thirring and Hardy–Lieb–Thirring Inequalities”, arXiv:2510.24148 (2025).

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