We present a Thomas-Fermi-inspired density scaling under which electron densities of atomic, molecular, or condensed matter become both large and slowly varying, so that semiclassical approximations and second-order density gradient expansions are asymptotically exact for the kinetic and exchange energies. Thus, even for atoms and molecules, density-functional approximations should recover the universal second-order gradient expansions in this limit. We also explain why common generalized gradient approximations for exchange do not.
Aaron D. Kaplan, Biswajit Santra, Puskar Bhattarai, Kamal Wagle, Shah Tanvir ur Rahman Chowdhury, Pradeep Bhetwal, Jie Yu, Hong Tang, Kieron Burke, Mel Levy, John P Perdew
Aaron D. Kaplan, Biswajit Santra, Puskar Bhattarai, Kamal C. Wagle, Shah Tanvir ur Rahman Chowdhury, Pradeep Bhetwal, Jie Yu, Hong Tang, Kieron Burke, Mel Levy, John P Perdew
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