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18.1.9 BR: Becke-Roussel Exchange Functional
A. D. Becke and M. R. Roussel,Phys. Rev. A 39, 3761 (1989)
 |
(47) |
where
 |
(48) |
 |
(49) |
and
is defined by the nonlinear equation
 |
(50) |
where
 |
(51) |
 |
(52) |
and
 |
(53) |
P.J. Knowles and H.-J. Werner
molpro@tc.bham.ac.uk
Jan 15, 2002