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. 2016 Mar 10;144(10):104304. doi: 10.1063/1.4942019

TABLE III.

Orbital occupations of the dominant spin-adapted determinants of the CASSCF(18,12)/ccpVTZ wave functions for the 11A1 and 21A1 states of O3.a

Active orbitalsd,e,f,g,h
Spin adapted determinantb,c 5a1 3b1 1b2 6a1 1a2 4b1 2b2 7a1 5b1 Excitation with respect to D1 or D2
D1 2 2 2 2 2 2
D2 2 2 2 2 2 2
D3 2 2 2 2 2 2 D1,(1a2)2(2b2)2
D4 2 2 2 2 2 2 D2,(6a1)2(4b1)2
D5 2 2 2 2 2 2 D2,(5a1)2(7a1)2
D6 2 2 2 2 2 2 D2,(1a2)2(5b1)2
D7 2 2 2 2 2 2 D2,(3b1)2(5b1)2
D8 2 2 1 2 2 2 1 D1,(1b2)2(1b2)1(2b2)1
D9 2 1 2 2 2 2 1 D2,(3b1)2(3b1)1(5b1)1
D10 1 2 2 1 2 2 2 D1,(5a1)2(6a1)2(5a1)1(6a1)1(2b2)2
D11 1 2 2 2 2 2 1 D2,(5a1)2(5a1)1(7a1)1
D12 2 2 2 1 2 2 1 D2,(6a1)2(6a1)1(7a1)1
a

Listed are the orbital occupations of the 1A1 spin-adapted determinants that occur in Table II. The spin-adapted determinants with singly occupied orbitals are normalized combinations of two Slater-determinants.

b

Indicated in bold font are the configurations, D1 and D2, that span the 1A1 subspace of the CAS(2,2).

c

Also indicated in bold are the configurations, D3 and D4, that, together with shaded D1 and D2, span the 1A1 subspace of the CAS(6,4).

d

The doubly occupied core orbitals 1a1, 1b1, and 2a1 are not listed.

e

For each of the dominant spin-adapted determinants that contribute to the 11A1 and 21A1 wave functions of O3, the valence orbitals 3a1, 2b1, and 4a1 are all doubly occupied and therefore not listed. However, the full CAS(18,12) space also contains determinants that involve excitations from orbitals 3a1, 2b1, and 4a1.

f

Indicated as shaded part are the active orbitals, 4b1 and 2b2, that have different occupations in D1 and D2.

g

Indicated in bold are the active orbitals, 6a1 and 1a2, that have different occupations in D3 and D4.

h

Orbitals of a1 and b1 symmetry are σ-type orbitals. Orbitals of a2 and b2 symmetry are π-type orbitals.