要旨
The cumulant 2-matrix chi is that part of the two-body reduced density matrix gamma2, which cannot be reduced to products of the one-body reduced density matrix (1-matrix) gamma. This irreducible part chi is calculated perturbatively for the high-density electron gas (EG) in its ground state, such that the pair densities and the interaction energy are correctly reproduced in their high-density limits, which are exactly known and summarized here. From the thus available cumulant 2-matrix the pair density in momentum space can be derived and used for a fluctuation analysis and compared with the analog analysis in position space, where it is concluded that "correlation suppresses fluctuations". The perturbatively available cumulant 2-matrix chi can be used also for the high-density electron gas to start the iterative solution of the Yasuda integral equation of density matrix functional theory (DMFT), which is a nonlinear functional relation between the cumulant 2-matrix chi and the 1-matrix gamma recently derived from the contracted Schrodinger equation approach: chi(gamma)[gamma]. From the perturbatively determined chi one can find another functional chi[gamma] as an alternative approximation for a DMFT. (C) 2002 Wiley Periodicals, Inc.
