Exact solution of the many-body problem with a O(n6)\mathcal{O}\left(n^6\right) complexity

Abstract

In this article, we define a new mathematical object, called a pair D=(A,C)D=\left(A,C\right) of anti-commutation matrices (ACMP) based on the anti-commutation relation ai†aj+ajai†=Ξ΄ija^\dag_{i}a_{j} + a_{j}a^\dag_{i} = \delta_{ij} applied to the scalar product between the many-body wavefunctions. This ACMP explicitly separates the different levels of correlation. The one-body correlations are defined by a ACMP D0=(A0,C0)D^0=\left(A^0,C^0\right) and the two-body ones by a set of nn ACMPs Di=(Ai,Ci)D^i=\left(A^i,C^i\right) where nn is the number of states. We show that we can have a compact and exact parametrization with n4n^4 parameters of the two-body reduced density matrix (\TRDM) of any pure or mixed NN-body state to determine the ground state energy with a O(n6)\mathcal{O}\left(n^6\right) complexity

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