A detailed derivation of excited-state energy gradients is presented.
The excited states are generated by singles-only configuration interac
tion (CIS) from the Hartree-Fock ground-state wave-function with a res
triction placed on the active space (RCIS). The derivative of the RCIS
equation is found using the CPHF equations. However, at this point, t
he RCIS gradient equation is not in its most computationally efficient
form. Therefore, the so-called Z-vector method is used to eliminate t
he dependence of the derivative equation on the orbital rotation matri
x U'. This is done by defining a ''Z vector,'' which for our case is M
e restricted one-particle density matrix. Its product with Me Q' matri
x is used to substitute for the terms which involve the orbital rotati
on matrix. Since the Z-vector is defined by the RCIS Lagrangian and th
e Lagrangian is redefined by the restriction on the active space, it i
s necessary to rederive the derivation equation in order to eliminate
unnecessary terms. Once U' has been eliminated, the derivative equatio
n may be written entirely in the AO basis. This avoids time-consuming
AO to MO transformations. (C) 1997 John Wiley & Sons, Inc.