Abstract
Using the classical gas expression for the diffusion coefficient and experimental measurements of the spin diffusion coefficient of a 5% solution of He3 in He4 at temperatures up to 1°K, we have extended the effective interaction between He3 quasiparticles, as derived by Bardeen, Baym, and Pines, to larger values of the momentum. This potential is then used in first-order perturbation theory to calculate the high-temperature magnetic susceptibility of dilute solutions and the variation in the He3 chemical potential with concentration. From the latter, and from measurement of the phase-separation curve at finite temperature, the maximum solubility of He3 in He4 is determined down to T=0. Agreement with experiment is good.

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