TY - JOUR
T1 - Characterization of the X 1A1 and à 1B2 electronic states of titanium dioxide, TiO2
AU - Wang, Hailing
AU - Steimle, Timothy
AU - Apetrei, Cristina
AU - Maier, John P.
PY - 2009/1/1
Y1 - 2009/1/1
N2 - The strong band system at 536 nm, tentatively assigned as the à 1B2← X 1A1(000-000) vibronic transition, in TiO2 has been recorded at a spectral resolution of 40 MHz, both field free and in the presence of a static electric field. The Stark induced shifts were analyzed to determine the permanent electric dipole moments of 6.33 ± 0.07 D and 2.55± 0.08 D for the X 1A1 and à 1B2 state, respectively. The bond angle, θ, and length, RTi-O, for the à 1B2 state were determined to be 100.1° and 1.704 Å. The dispersed fluorescence was analyzed to determine the ν2 bending frequency, ω2 (a1), of 322 ± 6 cm-1. A molecular orbital model is used to rationalize the change in bonding upon excitation and the results compared with electronic structure predictions.
AB - The strong band system at 536 nm, tentatively assigned as the à 1B2← X 1A1(000-000) vibronic transition, in TiO2 has been recorded at a spectral resolution of 40 MHz, both field free and in the presence of a static electric field. The Stark induced shifts were analyzed to determine the permanent electric dipole moments of 6.33 ± 0.07 D and 2.55± 0.08 D for the X 1A1 and à 1B2 state, respectively. The bond angle, θ, and length, RTi-O, for the à 1B2 state were determined to be 100.1° and 1.704 Å. The dispersed fluorescence was analyzed to determine the ν2 bending frequency, ω2 (a1), of 322 ± 6 cm-1. A molecular orbital model is used to rationalize the change in bonding upon excitation and the results compared with electronic structure predictions.
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U2 - 10.1039/b821849h
DO - 10.1039/b821849h
M3 - Article
C2 - 19421521
AN - SCOPUS:64549129163
SN - 1463-9076
VL - 11
SP - 2649
EP - 2656
JO - Physical Chemistry Chemical Physics
JF - Physical Chemistry Chemical Physics
IS - 15
ER -