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Physics Letters

The logarithmic term in the ground-state energy formula of a dilute fermi-gas of hard spheres

V.N. Efimov

Published Mar 1, 1965• 11 citations
Publisher
DOI
10.1016/0031-9163(65)91124-8

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The Lee-Huang-Yang energy for a dilute gas of hard spheres: an upper bound

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We consider a quantum gas consisting of $N$ hard spheres with radius $\frak{a} > 0$, obeying bosonic statistics and moving in the box $Λ= [0;L]^3$ with periodic boundary conditions. We are interested in the ground state energy per unit volume in the thermodynamic limit, with $N, L \to \infty$ at fixed density $ρ= N / L^3$. We derive an upper bound for the ground state energy density, matching the famous Lee-Huang-Yang formula, up to lower order terms, in the dilute limit $ρ\frak{a}^3 \ll 1$.

arXiv:2603.13084•Mar 13, 2026•0 citations
We consider a quantum gas consisting of NNN hard spheres with radius a>0\frak{a} > 0a>0, obeying bosonic statistics and moving in the box Λ=[0;L]3Λ= [0;L]^3Λ=[0;L]3 with periodic boundary conditions. We are interested in the ground state energy per unit volume in the thermodynamic limit, with N,L→∞N, L \to \inftyN,L→∞ at fixed density ρ=N/L3ρ= N / L^3ρ=N/L3. We derive an upper bound for the ground state energy density, matching the famous Lee-Huang-Yang formula, up to lower order terms, in the dilute limit ρa3≪1ρ\frak{a}^3 \ll 1ρa3≪1.