Abstract
A calculation of the correction, second order in $\frac{v}{c}$, to the binding energy of nuclear matter in the first-order Hartree-Fock approximation yields a result of +0.5 MeV per particle at ${k}_{F}=1.36$. The correction becomes large very quickly as the Fermi momentum increases. These results are based on the nonlocal separable potential of Tabakin.
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