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Phys. Rev. Lett. 49, 1691–1694 (1982)

Density-Functional Theory for Fractional Particle Number: Derivative Discontinuities of the Energy

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John P. Perdew
Department of Physics and Quantum Theory Group, Tulane University, New Orleans, Louisiana 70118

Robert G. Parr
Department of Chemistry, University of North Carolina, Chapel Hill, North Carolina 27514

Mel Levy
Department of Chemistry and Quantum Theory Group, Tulane University, New Orleans, Louisiana 70118

Jose L. Balduz, Jr.
Department of Physics, Carnegie-Mellon University, Pittsburgh, Pennsylvania 15213

Received 16 August 1982; published in the issue dated 6 December 1982

The Hohenberg-Kohn theorem is extended to fractional electron number N, for an isolated open system described by a statistical mixture. The curve of lowest average energy EN versus N is found to be a series of straight line segments with slope discontinuities at integral N. As N increases through an integer M, the chemical potential and the highest occupied Kohn-Sham orbital energy both jump from EM-EM-1 to EM+1-EM. The exchange-correlation potential δExc/δn(r⃗) jumps by the same constant, and limrδExc/δn(r⃗)>~0.

© 1982 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevLett.49.1691
DOI:
10.1103/PhysRevLett.49.1691
PACS:
31.10.+z, 71.45.Gm