Revision 2

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Changes against revision 1:

Title: Third-order term in the dilute Bose gas ground-state energy
Plain: The energy of a dilute repulsive Bose gas is known rigorously to two terms in powers of the density. The next predicted term, with a logarithm, is proven only from above.
Precise · changed · core: Revision 1: With $\hbar^{2}/(2m) = 1$, the ground-state energy density is predicted to be $e(\rho) = 4 \pi a \rho^2 [1 + (128/(15 \sqrt{\pi})) (\rho a^3)^{1/2} + 8 (4 \pi/3 - \sqrt{3}) \rho a^3 \operatorname{log}(\rho a^3) + o(\rho a^3 \operatorname{log}(\rho a^3))]$ (Wu, 1959). Prove the matching lower bound for general short-range $v \ge 0$. Answer: a proof of the two-sided expansion.; Revision 2: With $\hbar^{2}/(2m) = 1$, the ground-state energy density is predicted to be $e(\rho) = 4 \pi a \rho^2 [1 + (128/(15 \sqrt{\pi})) (\rho a^3)^{1/2} + 8 (4 \pi/3 - \sqrt{3}) \rho a^3 \log(\rho a^3) + o(\rho a^3 \log(\rho a^3))]$ (Wu, 1959). Prove the matching lower bound for general short-range $v \ge 0$. Answer: a proof of the two-sided expansion.
Settled by: A lower bound on $e(\rho)$ matching the Wu term.
Kind: well-posed
Answer type: proof
References: (empty)
Literature status: partially-resolved
Status note: The two-term Lee-Huang-Yang formula is proven (Yau and Yin 2009, upper bound; Fournais and Solovej 2020, lower bound); a third-order upper bound in the thermodynamic limit was proven by Brooks, Oldenburg, Saint Aubin and Schlein (arXiv 2506.04153, 2025).
Posed since: 1959

Decisions