Abstract
The partition function which Feynman has proposed for liquid He4 is extended to the case of liquid He3, taking into account the Fermi-Dirac statistics and the nuclear spin of ½. The nuclear magnetic susceptibility is calculated and compared with the observation of Fairbank, Ard, and Walters. Theoretical and experimental curves fit when the effective mass of the He3 atom is taken about four times its true mass. The entropy of the system has not been calculated.

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