Inhomogeneous Electron GasPhysical Review, Vol. 136, No. 3B. (November 1964), pp. B864-B871.
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AbstractThis paper deals with the ground state of an interacting electron gas in an external potential v (r). It is proved that there exists a universal functional of the density; F [ n (r)]; independent of v (r); such that the expression E ≡∫ v (r) n (r) d r+ F [ n (r)] has as its minimum value the correct ground-state energy associated with v (r). The functional F [ n (r)] is then discussed for two situations: (1) n (r)= n 0 + n ̃(r); n ̃ / n 0 ≪1; and (2) n (r)=ϕ(r / r 0 ) with ϕ arbitrary and r 0 →∞. In both cases F can be expressed entirely in terms of the correlation energy and linear and higher order electronic polarizabilities of a uniform electron gas. This approach also sheds some light on generalized Thomas-Fermi methods and their limitations. Some new extensions of these methods are presented.
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