Abstract
A theory of the normal ground state of liquid He3 is constructed using matrix elements in a representation of correlated basis functions. The Rayleigh-Schrödinger perturbation theory is adapted to our nonorthogonal basis. Several means of classifying terms are avaiable; one of them is recognized as best suited for the study of liquid He3. To the second order in the classification scheme, the following ground-state properties are calculated and compared with experiment and results of the Brueckner-Gammel theory: energy per particle, equilibrium density, compressibility, velocity of sound, and paramagnetic susceptibility. The radial distribution function of liquid He3 at zero temperature is also calculated. A study of the Löwdin transformation as a procedure for orthogonalizing the correlated basis shows that the correction to the Hamiltonian involves unphysical N dependences; these arise out of high-order irreducible clusters and unlinked diagrams. It is verified that the unphysical terms cancel out completely in each of several lowest orders.