Abstract

Abstract By applying the variational principle to the grand potential including residual two-body interactions, the thermal random-phase-approximation (TRPA) equation is derived without recourse to the linearization ansatz. The relation of the TRPA equation to the stability condition of the thermal Hartree-Fock-Bogoliubov (THFB) solution is elucidated.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call