An asymptotically corrected (AC) exchange potential proposed by van Leeuwen and
Baerends is
1292
Phys. Rev. A
(1994),
49,
pp. 2421.
Link
(5.64) |
where is the reduced
density gradient. For an exponentially-decaying density, this potential
reduces to in the asymptotic region of molecular systems. The LB94 xc
potential is formed by a linear combination of LDA XC potential and the LB
exchange potential:
1292
Phys. Rev. A
(1994),
49,
pp. 2421.
Link
(5.65) |
The parameter in Eq. (5.64) was determined by fitting to the
exact XC potential for Be atom. As mentioned in Refs.
196
J. Chem. Phys.
(1998),
108,
pp. 4439.
Link
and
542
Chem. Phys. Lett.
(1999),
314,
pp. 291.
Link
, for TDDFT calculations, it is sufficient to
include the AC XC potential for ground-state calculations followed by TDDFT
calculations with an adiabatic LDA XC kernel. The implementation of the LB94 XC
potential in Q-Chem takes this approach, using the LB94 XC potential for the
ground state calculations, followed by a TDDFT calculation with an adiabatic
LDA XC kernel. This TDLDA/LB94 approach has been widely applied to study
excited-state properties of large molecules.
Since the LB exchange potential in Eq. (5.64) does not come from the
functional derivative of an exchange energy functional, the Levy-Perdew virial
relation
766
Phys. Rev. A
(1985),
32,
pp. 2010.
Link
is used instead to obtain the exchange energy:
(5.66) |
An LB94 calculation is requested by setting EXCHANGE = LB94 in the $rem section. Additional job control and examples appear below.
LB94_BETA
LB94_BETA
Sets the parameter for the LB94 XC potential
TYPE:
INTEGER
DEFAULT:
500
OPTIONS:
Corresponding to .
RECOMMENDATION:
Use the default.
$comment TDLDA/LB94 calculation is performed for excitation energies. $end $molecule 0 1 N 0.0000 0.0000 0.0000 N 1.0977 0.0000 0.0000 $end $rem EXCHANGE lb94 BASIS 6-311(2+,2+)G** CIS_N_ROOTS 30 RPA true $end