Near each nucleus of a heavy atom or molecule, the true ground-state electron density is close, with explicit L^p error bounds, to the density of a single non-interacting hydrogenic atom, in both nonrelativistic and relativistic settings.
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Strong Scott Conjecture
Near each nucleus of a heavy atom or molecule, the true ground-state electron density is close, with explicit L^p error bounds, to the density of a single non-interacting hydrogenic atom, in both nonrelativistic and relativistic settings.