Abstract
A system of N antisymmetric particles, moving under the influence of a fixed potential and their mutual many-particle interactions, is investigated in the ordinary Hartree-Fock scheme, having the total wave function approximated by a single Slater determinant. It is shown that all the density matrices of various orders, the wave function, and the entire physical situation depends only on a fundamental invariant ρ(x1, x2), which is identical with the first-order density matrix. The Hartree-Fock equations are expressed in terms of this quantity.

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