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PRINT MOS SCFTYPE UKS MOMODIFY 0 1 1 0.75 GEOMETRY CARTESIAN ANGSTROM He 0.0 0.0 0.0
Note that the MULTIPLICITY keyword (see 4.4.1) refers to the unmodified system, i.e. without fractional MO occupation. The fractional MO occupation can be best monitored by printing the molecular orbitals. We find for the above He atom input after SCF convergence:
ALPHA MO COEFFICIENTS OF CYCLE 6 1 2 -0.7814 0.3711 1.0000 0.0000 1 1 He 1s 0.8294 -0.9999 2 1 He 2s 0.2402 1.2768 BETA MO COEFFICIENTS OF CYCLE 6 1 2 -0.7342 0.3936 0.7500 0.0000 1 1 He 1s 0.8089 -1.0166 2 1 He 2s 0.2661 1.2716
As this output shows the 0.75 occupation of the MO breaks the
energy degeneracy of the
and
MOs. Also the MO coefficients are
different. To obtain total energies that match with integer occupied
calculations, e.g. for the cation or anion, the UKS SCFTYPE
(see 4.5.1) option must be selected!