Abstract
This paper is the first of two in which the coupled cluster method (CCM) or exp(S) formalism is applied to two-component Fermi systems, the aim being to describe real metals and superconductivity. In this paper we concentrate on exact results and restrict ourselves to a ring approximation, applicable essentially to a high-density regime. We show that in the ground-state formalism the random phase approximation (RPA) can be formulated as a system of coupled, bilinear integral equations satisfied by functions associated with the so-called four-point functions of the system which provide a measure of the two-particle-two-hole component in the true ground-state wavefunction. These equations are analysed in the dimensionless parameter formed by the ratio of the species masses and exact analytic solutions obtained. For Coulombic potentials (V11V22 = V122) we show that the exact analytic solution is unique and obtain an expression for the correlation energy. For non-Coulombic potentials (V11V22 ≠ V122) we indicate how to obtain a possible analytic solution. An RPA-like treatment of the one- and two-body equations in the excited-state formalism is provided for completeness.
Original language | English |
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Pages (from-to) | 4203-4236 |
Number of pages | 34 |
Journal | Journal of Physics A: Mathematical and General |
Volume | 20 |
DOIs | |
Publication status | Published - 1987 |