A Coulomb ground-state density without Kohn-Sham ensemble representation
We construct a finite three-electron Coulomb molecule whose spin-summed ground-state density cannot be reproduced by any ground-state ensemble of noninteracting electrons in a single real, spin-independent local potential in $L^{3/2}(\mathbf R^3)+L^\infty(\mathbf R^3)$. The molecule has two equal positive integer nuclear charges, specified by an exact finite nonnumerical formula.
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