MCLR computes response calculations on single and multiconfigurational SCF wave functions. One of the basic uses of MCKINLEY and MCLR is to compute analytical hessians (vibrational frequencies, IR intensities, etc). MCLR can also calculate the Lagrangian multipliers for a MCSCF state included in a state average optimization and construct the effective densities required for analytical gradients of such a state. The use of keyword RLXRoot in the RASSCF program is previously required. We postpone futher discussion about MCLR to section 3.22.
It follows an example of how to compute the analytical hessian of an excited state:
&SEWARD &END Title p-benzoquinone anion. Casscf optimized geometry. Symmetry X Y Z Square Basis set C.ANO-L...4s3p2d. C1 .0000000000 2.2783822672 1.3271399214 C2 .0000000000 .0000000000 2.7374556550 nd of basis Basis set H.ANO-L...3s2p. H1 .0000000000 4.0361650878 2.3432668589 End of basis Basis set O.ANO-L...4s3p2d. O1 .0000000000 .0000000000 5.1965257318 End of basis End of Input &SCF &END TITLE p-benzoquinone(-) D2h OCCUPIED 8 2 5 1 7 1 4 0 ITERATIONS 40 END OF INPUT &RASSCF &END TITLE p-benzoquinone anion. 2B3u state. SYMMETRY 2 SPIN 2 NACTEL 9 0 0 INACTIVE 8 0 5 0 7 0 4 0 RAS2 0 3 0 1 0 3 0 1 CIROOT 1 1 1 ITER 50,25 LUMORB END OF INPUT &ALASKA &END End of input &MCKINLEY &END Perturbation Hessian End of input &MCLR &END Thre 0.0001 Print 255 Rassi Elec End of input
Keyword ELECtric computes the gradient of the dipole moment. Combined with keyword RASSi, which is used to transform the CI vectors to split GUGA representation and the orbital rotations to AO basis to make the response accessible for state interaction calculations, it allows to compute the transition dipole moment geometry derivatives for further uses.