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Journal of Low Temperature Physics

Dynamic Susceptibility of the Free Fermi Gas in 2D

E. Sola, A. Polls, Ferran Mazzanti

Published Apr 1, 2002• 0 citations
Publisher
DOI
10.1023/a:1014745020960

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Nuclear magnetic susceptibility measurements of the $^{3}\mathrm{He}$ in dilute $^{3}\mathrm{He}$-$^{4}\mathrm{He}$ mixture films are presented. At low $^{3}\mathrm{He}$ coverages (${d}_{3}<0.1$ layer), the $^{3}\mathrm{He}$ behaves approximately as a 2D ideal Fermi gas. For larger submonolayer $^{3}\mathrm{He}$ coverages, the low-temperature susceptibility is enhanced, increasing with increasing amounts of $^{3}\mathrm{He}$, contrary to the 2D ideal Fermi-gas model. No evidence for a phase transition in the $^{3}\mathrm{He}$ is seen.

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The thermodynamic properties of a nonrelativistic free-electron Fermi gas is of fundamental interest in condensed matter physics. Properties previously studied in three-dimensions (3D) in the low- and high-temperature limits include the internal energy, heat capacity, zero-field magnetic spin susceptibility, and pressure. Here we report solutions for the temperature dependence spanning these two temperature regimes of the chemical potential, internal energy, magnetic susceptibility, and the heat capacity at constant volume in 1D, 2D, and 3D. Also calculated are the pressure, enthalpy, heat capacity at constant pressure, isothermal compressibility, and thermal expansion coefficient versus temperature in 2D and 3D. Of primary interest here are the detailed dimension-dependent crossovers of these properties between the degenerate and nondegenerate temperature regime, which are graphically illustrated for each of the above properties.
Nuclear magnetic susceptibility measurements of the 3He^{3}\mathrm{He}3He in dilute 3He^{3}\mathrm{He}3He-4He^{4}\mathrm{He}4He mixture films are presented. At low 3He^{3}\mathrm{He}3He coverages (d3<0.1{d}_{3}<0.1d3​<0.1 layer), the 3He^{3}\mathrm{He}3He behaves approximately as a 2D ideal Fermi gas. For larger submonolayer 3He^{3}\mathrm{He}3He coverages, the low-temperature susceptibility is enhanced, increasing with increasing amounts of 3He^{3}\mathrm{He}3He, contrary to the 2D ideal Fermi-gas model. No evidence for a phase transition in the 3He^{3}\mathrm{He}3He is seen.