Remember that [G.sub.F] is the Fermi coupling constant, [C.sub.A] [equivalent] 1.26 is the axal-vector weak coupling constant of a neutron, and [N.sub.v] = 3 is the number of neutrino flavors; [p.sub.F] is the Fermi momentum
of neutrons, [m.sup.*] = [p.sub.F] / [v.sup.F] is the effective neutron mass; m is bare nucleon mass, [T.sub.9] = T/([10.sup.9]K), [k.sub.B] is the Boltzmann constant, and
Lately, in order to reduce the effect of the high-momentum component of strong nuclear force on finite nuclei properties, a Fermi momentum cutoff has been imposed on both average effective interactions and density- and channel-dependent ones [76, 77].
It should be noted that k's are topped to the Fermi momentum, [K.sub.F]([rho]) = [(6[[pi].sup.2][rho]/v).sup.1/3], with v being degeneracy parameter of nucleons.
Mariji, "Imposing Fermi momentum cut-off on the channel-and density-dependent effective interaction and the groundstate properties of closed shell nuclei," The European Physical Journal A, vol.
Modarres, "The effect of Fermi momentum cutoff on the binding energy of closed shell nuclei in the LOCV framework," Physics of Particles and Nuclei Letters, vol.
This leads to a spectrum that is continuous at the Fermi momentum, which provided the name "continuous choice" for this approach.
The Pauli operator Q([p.sub.1], [p.sub.2]) restricts the intermediate states to particle states with momenta [p.sub.1], [p.sub.2], which are above the corresponding Fermi momentum. However, the single-particle spectrum is often parameterized in the form of an effective mass
The corrections of the single-particle energies due to the [DELTA][[summation].sup.2h1p] term are larger for momenta below the Fermi momentum and tend to zero for momenta above [k.sub.F].