Theor Chem Acc (2015) 134:148
1 3
In the present work, the exchange contribution, which
is present only in the case of Hartree–Fock or hybrid density functional fockians and which would give rise to nonconventional two-electron integrals, is not treated explicitly. Possible approximate solutions for this problem will
be discussed in forthcoming works. Although we do not
use the elements of the off-diagonal ( i = j ) blocks of the
POO fock operator, for the sake of completeness we give
its expression:
To derive this, instead of the double commutator of
Eq. 73 , one needs to consider the product of the commutator with a coordinate operator
where ˆ
T is the kinetic energy operator, and [ˆ r β , ˆ
T ] = ˆ
∇ β .
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i α | ˆ
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