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Thermal effects in the ultrafast photoinduced electron transfer from a molecular donor anchored to a semiconductor acceptor
Author(s) -
Stier William,
Prezhdo Oleg V.
Publication year - 2003
Publication title -
israel journal of chemistry
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.908
H-Index - 54
eISSN - 1869-5868
pISSN - 0021-2148
DOI - 10.1560/u3gf-g11x-325d-0wj1
Subject(s) - chemistry , photoexcitation , excited state , delocalized electron , acceptor , electron transfer , photoinduced electron transfer , adiabatic process , molecular physics , molecular dynamics , atomic physics , chromophore , chemical physics , ionic bonding , ion , computational chemistry , photochemistry , thermodynamics , physics , condensed matter physics , organic chemistry
A nonadiabatic molecular dynamics (MD) simulation of the photoinduced electron transfer (ET) from a molecular electron donor to the TiO 2 semiconductor acceptor is carried out in a microcanonical ensemble with an average temperature of 350 K. The electronic structure of the dye–semiconductor system and the adiabatic dynamics are simulated by ab initio MD, while the nonadiabatic (NA) effects are incorporated by a quantum‐classical mean‐field approach. The ET dynamics are driven by thermal fluctuations that dominate ionic motions at the simulated temperature. The ground and excited state ion dynamics are similar; therefore, the change in the quantum force due to the electronic photoexcitation can be neglected, and the analysis is greatly simplified. The simulated ET occurs on a 5‐fs timescale, in agreement with recent ultrafast experimental data. Vibrational motions of the chromophore ring carbons induce an oscillation of the photoexcited state energy, resulting in a bimodal distribution of the initial conditions for ET. At low energies the photoexcited state is localized primarily on the chromophore, while at high energies the photoexcited state is substantially delocalized into the TiO 2 surface. Thermally driven adiabatic transfer is the dominant ET mechanism. Compared to the earlier simulation at 50 K, the rate of NA transfer at 350 K remains almost unchanged, whereas the rate of adiabatic ET increases substantially.