Abstract
We have measured the solubility of 4 He in liquid 3 He down to about 40 mK and at pressures from zero up to ∼ 24 atm. The solubility was obtained from the thickness of the superfluid film in contact with unsaturated solutions of 4 He in 3 He as a function of temperature. By fitting the solubility data to Fermi liquid theory, we obtained the parameters m *4 and Δ as a function of pressure. Here, m *4 is the effective mass of 4 He in liquid 3 He and Δ the difference in binding energy between 4 He in pure 4 He and 4 He in liquid 3He. This difference has a minimum near 10 atm. The average of the results for m *4 , at different pressures, is (1.3 ± 0.2)m 4. This agrees with the many body calculations of de Saavedra et al., and with the Stokes hydrodynamic mass using the partial volume of 4 He in 3 He, v *4 . The partial volume was obtained by taking the derivative of Δ with respect to pressure.
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He, J., Culman, T.G., Hjort, H.H. et al. The Effective Mass and Binding Energy of 4He in 3He in the Fermi Liquid Region. Journal of Low Temperature Physics 113, 987–992 (1998). https://doi.org/10.1023/A:1022544015141
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DOI: https://doi.org/10.1023/A:1022544015141