The precise relationship between the exact expressions for the Kohn–Sham exchange-correlation potential, ,
deduced by Buijse, Baerends and Snijders and by Ryabinkin, Kohut and
Staroverov is clarified. These two expressions differ nontrivially by a
single term which in the former method generally involves the
three-electron reduced density matrix, whereas in the latter approach
the same term is expressed using the two-electron reduced density matrix
at most. The link between the two expressions turns out to be the
1,3-contracted Schrödinger equation. An essential feature of these and
other similar expressions for
is that they produce different results in finite-basis-set calculations and become equivalent only in the basis-set limit.
https://sci-hub.se/https://doi.org/10.1080/00268976.2018.1463470
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