Journal Article10.1103/PHYSREVB.31.2719
Phase transition of two-dimensional He 3 from a dilute to a dense phase
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TL;DR: Two puzzling aspects of the results are the lack of a significant heat-capacity jump at the transition and, based on a linear extrapolation of the data to zero temperature, a substantial amount of missingmore » entropy.
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Abstract: We have measured the heat capacity of $^{3}\mathrm{He}$ in films of $^{4}\mathrm{He}$ as thin as 10 A\r{} formed on a Nuclepore filter substrate. At low temperatures, where the $^{3}\mathrm{He}$ is in the lowest state as far as motion perpendicular to the film surface, we find that the $^{3}\mathrm{He}$ undergoes a transition from a dilute phase to a dense phase. We have observed this transition for films of $^{4}\mathrm{He}$ of 12.3- and 10-A\r{} thickness and for coverages of $^{3}\mathrm{He}$ below about 0.2 atomic layers. For thicker $^{4}\mathrm{He}$ films, and higher $^{3}\mathrm{He}$ coverages, the $^{3}\mathrm{He}$ remains homogeneously spread out over the surface of the $^{4}\mathrm{He}$. The striking characteristic of the transition is the sudden onset of linear temperature dependence with a slope which is proportional to the amount of $^{3}\mathrm{He}$ in the calorimeter. This is consistent with the formation of islands of a dense two-dimensional phase which grows in extent proportionately to the amount of $^{3}\mathrm{He}$. Two puzzling aspects of our results are the lack of a significant heat-capacity jump at the transition and, based on a linear extrapolation of the data to zero temperature, a substantial amount of missing entropy.
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Citations
Kohn-Luttinger effect and the instability of a two-dimensional repulsive Fermi liquid at T =0
TL;DR: In the dilute limit, numerical studies show that the Kohn-Luttinger effect survives down to l=1 and gives rise to a p-wave pairing and the relevance of these results to experiments on He adsorbed on the free surface of He is discussed.
158
Effect of 3He on submonolayer superfluidity.
Gabor Csathy,Moses H. W. Chan +1 more
TL;DR: The T = 0 superfluid-insulator phase boundary, which can be described by a simple function, is found in the 3He-4He coverage plane.
98
Near-monolayer 3He-4He films: Two superfluid transitions and the 3He effective mass and binding energy.
Xingwu Wang,Francis M. Gasparini +1 more
TL;DR: It is found that the effective mass has a maximum as a function of /sup 4/He thickness with correct asymptotic values for infinite and zero thickness limits, and this maximum coincides very nearly with the thickness of /Sup 4/ he at which the transition into the superfluid state takes place in two steps.
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References
•Book
Progress in Low Temperature Physics
D. F. Brewer,C. J. Gorter,William P Halperin,誠 坪田 +3 more
- 01 Jan 1964
TL;DR: In this article, the specific heat of high-T c superconductors was studied. But the authors focused on the scaling of 3 He-4 He mixtures and did not consider the properties of the order parameter collective modes of these mixtures.
2K
Superfluidity and phase separation in helium films
A. N. Berker,David R. Nelson +1 more
TL;DR: In this article, a vectorial generalization of the Blume-Emery-Griffiths model is proposed to describe superfluidity in films of pure 4-mathrm{He}$ mixtures and solved by an approximate renormalization scheme due to Migdal.
196
/sup 3/He in /sup 4/He films: Homogeneous two-dimensional behavior
TL;DR: In this paper, the authors report measurements and analysis of the heat capacity of /sup 3/He in /sup 4/He and show that the surface effective mass and excitation energy are functions of coverage and thickness.
74
Observation of two-dimensional phase separation in /sup 3/He-/sup 4/He films
TL;DR: In this article, the heat capacity of /sup 3/He adsorbed on /sup 4/He films was investigated and it was found that phase separation in the two-dimensional layer at the surface of the film was very sudden onset of degeneracy.
73
Propagation of surface sound in superfluid 3 He - 4 He
TL;DR: In this paper, a least-squares fit to the model was used to obtain the binding energy, the effective mass, and some limits on the sign and magnitude of the effective interaction between the quasiparticles.
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