ABSTRACT
It is known that the asymptotic decay of the electron density outside a molecule is informative about its first ionisation potential I0, . This dictates the orbital energy of the highest occupied Kohn–Sham (KS) molecular orbital (HOMO) to be εH = −I0, if the KS potential goes to zero at infinity. However, when the KS HOMO has a nodal plane, the KS density in that plane will decay as . Conflicting proposals exist for the KS potential: from exact exchange calculations it has been found that the KS potential approaches a positive constant in the plane, but from the assumption of isotropic decay of the exact (interacting) density, it has been concluded this constant needs to be negative. Here, we show that either (1) the exact density decays differently (according to the second ionisation potential I1) in the HOMO nodal plane than elsewhere, and the KS potential has a regular asymptotic behaviour (going to zero everywhere) provided that εH − 1 = −I1; or (2) the density does decay like everywhere but the KS potential exhibits strongly irregular if not divergent behaviour around (at) the nodal plane.
GRAPHICAL ABSTRACT
Acknowledgments
It is our pleasure to dedicate this paper to Andreas Savin, who always enjoyed to discover strange features in the Kohn–Sham potential and has been a pioneer in asking fundamental questions in exact DFT.
We thank the Netherlands Science Foundation NWO for a visitors grant for Tamás Gál and a Vidi grant for Paola Gori-Giorgi, and the WCU (World Class University) program of the Korea Science and Engineering Foundation (Project No. R32-2008-000-10180-0) for support. Paola Gori-Giorgi acknowledges useful discussions with A. Görling and S. Kümmel.
Disclosure statement
No potential conflict of interest was reported by the authors.