This section deals with the calculation of the
term of magnetic circular dichroism
for a dipole-allowed transition between the ground state
and
the excited state
.
The
term results from an appropriate combination of
products of electric dipole one-photon transition moments
and mixed electric dipole-magnetic dipole
two-photon transition moments--
or, more precisely, a combination of transition strengths
--
which are related to the single residues of the (linear and)
quadratic response functions [17,190,191]:
LABELA,LABELB,LABELC
are automatically specified.
Operator triples which do not correspond to symmetry-allowed
combinations will be ignored during the calculation.
This is the default.
READ (LUCMD,'(3A)') LABELA, LABELB, LABELC
DO WHILE (LABELA(1:1).NE.'.' .AND. LABELA(1:1).NE.'*')
READ (LUCMD,'(3A)') LABELA, LABELB, LABELC
END DO
Manually select the operator label triplets defining the operator
Cartesian components involved in the term.
The first two operators
(LABELA,LABELB)
are those that enter the two-photon moment.
The third operator (LABELC)
is the one that enters the one-photon
moment. They could be any of the (one-electron)
operators for which integrals are available in
**INTEGRALS.
Specifically for the term,
LABELA
corresponds to any component of the electric dipole
moment operator, LABELB
a component of the
angular momentum (magnetic dipole) and
LABELC
to a component of the electric dipole.
Operator triples which do not correspond to symmetry allowed
combination will be ignored during the calculation.
READ (LUCMD,*) IPRINT
IPRINT=0
.
READ (LUCMD,'(A70)') LABHELP
DO WHILE (LABHELP(1:1).NE.'.' .AND. LABHELP(1:1).NE.'*')
READ(LABHELP,*) IXSYM,IXST
END DO
Manually select one or more given excited states among those specified
in *CCEXCI.
The symmetry (
IXSYM
) and state number (IXST
)
within that symmetry are then given,
one pair (IXSYM,IXST
) per line.
Default is all dipole allowed states for all symmetries
specified in *CCEXCI.