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As reference determinants in the MRD-CI calculations we chose the determinants most strongly contributing to a single and double CI description of the dominant one- and two-photon states. These are (i) the SCF determinant; (ii) a determinant in which an electron has been promoted from the HOMO to the LUMO; (iii) one in which an electron has been excited from the HOMO-1 to the LUMO; (iv) the doubly excited determinant in which both electrons are excited from the HOMO to the LUMO; and (v) for molecule 1 the HOMO to LUMO+1 and for molecule 2 the HOMO to LUMO+5 determinants. The CI active space for the single excitations included the 24 highest occupied and 24 lowest unoccupied orbitals in molecule 1; for molecule 2, it was increased to 28×28 orbitals due to the larger number of π electrons. For the higher excitations, in all cases five occupied and five unoccupied orbitals have been considered.
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53
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59
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85099525973
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(3) and γ can be found in Ref. 39.
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Pacher, P.1
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4344611540
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The factor 1/5 is obtained for an isotropic medium assuming that the transition dipoles and state-dipole changes are parallel.
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68
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4344682043
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The quantum-chemical calculations reveal that the peak at 4.06 eV is, in fact, a superposition of 2PA into several excited states. Only the strongest of those states (the one used for the analysis in Table IV) displays any significant coupling to the higher-lying intermediate states. Therefore, for this 2PA-active state, a small underestimation of ISRE by the essential-state model can be expected while the contributions of the other 2PA-active states to the ISRE are better described by the essential-state model.
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