Calculation of third order properties
as quadratic response
functions.
,
, and
-named options refer to the operators in the quadratic
response function
[164,166,167]
The second order properties from the linear response functions
are also printed
(if
and
operators have the same spin symmetry),
as they can be obtained at no extra computational cost.
READ(LUCMD,'( A )')LABEL
Note that giving the label ANGMOM
, 1SPNORB
,
2SPNORB
, or MNFSPNOR
, all the components of angular
momentum, one-electron spin-orbit, two-electron spin-orbit or the
atomic mean-field spin-orbit operator will be selected.
By specifying the labels FERMI CO
, SPIN-DIP
or
PSO
, all components of the Fermi contact, spin-dipole or
paramagnetic spin-orbit integrals that can be found on the file
AOPROPER
will be selected. These integrals are selected by the
appropriate keywords in the **INTEGRALS input module.
READ(LUCMD,*)ISPINA
READ (LUCMD,*) NBQRFR
READ (LUCMD,*) (BQRFR(J),J=1,NBQRFR)
READ *, NFREQ
READ *, FREQ(1:NFREQ)
READ *, ISPINA,ISPINB,ISPINC
READ *,IPRHYP
READ(LUCMD,*) IAABB