Abstract
It is expected that a He3 atom in solid He4 travels through the lattice due to the tunneling effect and behaves as a quasi-particle, “impuriton”. We calculate the spin diffusion coefficient D of impuritons, using a realistic interaction between impuritons and obtain D\simeq(J34a)2⁄xV0, where J34 is the He3–He4 exchange constant, a the lattice constant, x the concentration of He3 impurities and V0 the strength of the interaction. It is shown that J34 is the same order of magnitude as the He3–He3 exchange constant in pure He3 solid at the same molar volume.