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I want to compute different contributions in the oscillator strengths from RASSI i.e., electric-dipole-electric-dipole, electric-quadrupole-electric-quadrupole, magnetic-dipole-magnetic-dipole, electric-dipole-electric-octupole, electric-dipole-magnetic-quadrupole.
It will be helpful if someone will explain how to read that in the output as well.
Does the QIALL keyword print all the quadrupole moments, electric as well as magnetic?
I don't understand how to get their individual contribution.
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QIALL should print all, but you also need to make sure you have included all required integrals (OMQI, MULT = 3), and possibly that all have the same origin (it should be the case by default, but in the case of charged systems, the dipole is not invariant and uses a different center). Example:
&GATEWAY
Coord = 4
angstrom
C 0.00000000 0.00000159 0.02308959
S -0.00000000 -0.00000053 1.66405025
H 0.93594257 -0.00000053 -0.56306999
H -0.93594257 -0.00000053 -0.56306999
Basis = ANO-RCC-MB
Group = NoSym
RICD
ANGM = 0.0 0.0 0.0
OMQI = 0.0 0.0 0.0
&SEWARD
Multipoles = 3
Center = 4
0 0.0 0.0 0.0
1 0.0 0.0 0.0
2 0.0 0.0 0.0
3 0.0 0.0 0.0
&RASSCF
nActEl=4
Charge = 0
SPIN = 1
RAS2 = 6
StAverage = 3
&RASSI
EJOB
QIAll
QIPrint = 0.0
In the output, you'll have:
1a. Dipole transition strengths
1b. Velocity transition strengths
2. Magnetic-Dipole - Magnetic-Dipole transition strengths
3. Quadrupole transition strengths
4. Electric-Dipole - Electric-Octupole transition strengths
5. Electric-Dipole - Magnetic-Quadrupole transition strengths
For convenience, you also have
6. Second-order contribution to the transition strengths (sum of 2-5)
So (if I'm not mistaken), the final strengths would be 1b+6. You could take 1a+6, but then you'd be mixing different gauges and the result wouldn't be origin-independent (see https://doi.org/10.1016/j.cplett.2017.05.003).
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