For fixed electron-electron interaction and electron number, a nondegenerate ground-state electron density determines the external potential up to an additive constant, and hence determines the Hamiltonian and ground-state observables.
Suppose two potentials differing by more than a constant have different ground states but the same density . Strict Rayleigh-Ritz variational principle inequalities give
Adding produces the contradiction . This proves the first Hohenberg-Kohn theorem under the stated nondegeneracy assumptions. A constant potential shift changes energy by times that constant without changing the density.[ref]

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