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. Author manuscript; available in PMC: 2014 May 16.
Published in final edited form as: J Phys Chem C Nanomater Interfaces. 2013 May 16;117(19):9673–9692. doi: 10.1021/jp311076w

Table 2.

Featured electronic transitions. The featured electronic transitions are presented for undoped and doped models. The criterion for selecting the states is the vicinity of the transition energy to the bandgap, large value oscillator strength, and potential to contribute to the charge transfer. Indices of doped orbitals are indicated with prime sign. Bright excitations are enlabeled in accordance with Fig. 1(c). Cartesian projections are included to identify the transitions of similar symmetry.

index description orbital pairs main data cartesian projections
hole
index
electron
index
oscillator
strength
transition
energy, eV
< 010 >
Dx
< 001 >
Dy
< 100 >
Dz
Undoped (100) TiO2 anatase + H2O, HO = 288
1 Bright, 1st HO−7 LU 3.40182621 2.4003 −4.3875 0.1813 0.0025
2 Bright, 2nd HO−8 LU+3 3.01603938 2.7111 −0.0317 −0.0648 3.8899

Ru-doped (100) TiO2 anatase + H2O, HO′ = 292
1′ Charged, Ru → slab HO′−2 LU′+4 0.89327673 1.3504 0.0887 −0.7205 −2.9109
2′ Bright, 1st analog HO′−10 LU′+2 2.16722662 2.5076 −3.4274 −0.0128 0.1078
3′ Bright, distortion-due HO′−7 LU′+3 2.74285120 2.5915 3.7948 −0.0099 −0.0044
4′ Bright, 3rd analog HO′−21 LU′+2 1.98818034 2.8562 −0.0275 −0.3825 3.0535
5′ Bright, 2nd analog HO′−11 LU′+4 1.46676219 2.8725 0.0729 −0.0262 2.6347
6′ Charged, slab → Ru HO′−13 LU′+1 0.18207940 2.1087 −1.0814 −0.0715 −0.0169
7′ Neutral, Ru → Ru HO′−2 LU′+1 0.18397963 0.5293 0.1680 −0.3840 2.1339