Abstract
We prove that the ground state energy of an atom confined to two dimensions with an infinitely heavy nucleus of charge and quantum electrons of charge -1 is $E(N,Z)=-{1/2}Z^2\ln Z+(E^{\TF}(λ)+{1/2}c^{\rm H})Z^2+o(Z^2)$ when and , where $E^{\TF}(λ)$ is given by a Thomas-Fermi type variational problem and is an explicit constant. We also show that the radius of a two-dimensional neutral atom is unbounded when , which is contrary to the expected behavior of three-dimensional atoms.
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