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Photophysics and photochemical dynamics of methylanisole molecules in a supersonic jet
Affiliation:1. School of Electronic and Information Engineering, Beihang University, Beijing 100191, China;2. Laboratory for Optoelectronics, Huazhong University of Science and Technology, Wuhan 430074, Hubei, China;3. School of Electronic Engineering, Southeast University, Nanjing 210096, Jiangsu, China;1. Max Planck Institute for Polymer Research, Ackermannweg 10, 55128 Mainz, Germany;2. Department of Radiology, Johannes Gutenberg University Medical Center, Langenbeckstr. 1, 55131 Mainz, Germany;1. Genentech, Drug Metabolism and Pharmacokinetics, 1 DNA Way, South San Francisco, CA 94080, United States;2. Genentech, Clinical Pharmacology, 1 DNA Way, South San Francisco, CA 94080, United States;3. Covance Laboratories, 3301 Kinsman Blvd., Madison, WI 53704, United States;1. Institute of Physical and Organic Chemistry, Southern Federal University, Stachki Av., 194/2, 344090, Rostov-on- Don, Russian Federation;2. Department of Chemistry, Southern Federal University, Zorge st., 7, Rostov-on-Don, 344090, Russian Federation;3. Hewlett Packard Enterprise (HPE), Moscow, Leningradskoe Highway 16a, p. 3, 125171, Russian Federation
Abstract:The fluorescence excitation, dispersed fluorescence and hole burning spectra, and fluorescence lifetimes of jet-cooled o-, m-, and p-methylanisoles (MA) were measured. The low-frequency ring methyl internal rotational bands observed for their S0 and S1 states were assigned. In the case of m-MA, the rotational isomers of cis and trans conformers, which arise from the orientation of the OCH3 group with respect to the CH3 group, were assigned by hole-burning spectroscopy. The observed level energies and relative intensities of the methyl internal rotation were reproduced by a calculation using a free rotor basis set. Furthermore, their potentials in the S0 and the S1 states were determined. The potential barrier heights for the S0 states of m- and p-MA were quite low, suggesting that the methyl groups are freely rotating, while changing from S0 to S1 states, the potential barrier height increases. The potential barrier heights of o-MA drastically decreased in going from S0 to S1 states. The decrease would be due to the hydrogen bonding between O atom and one H atom of the methyl group. The torsional bands of the methoxy group (–OCH3) were also observed for p- and o-MA. The –OCH3 modes are found to couple with the level of the e species for the methyl internal rotation.Fluorescence lifetimes (τf) of the methyl internal rotational bands in the S1 states of o-, m-, and p-MA were measured in order to investigate the photochemical dynamics. The values of the nonradiative rate constant (knr) were estimated from the τf values and Franck–Condon factors. The knr values drastically increased with the excitation of methyl internal rotation. Accordingly, the methyl internal rotation should enhance the nonradiative process, presumably intersystem crossing (ISC). The enhancement should be caused by the increase of the state density (ρ) effectively coupled with triplet manifolds. The drastic increase in the ρ value should be caused by level mixing. In addition, the methyl internal rotational motion may enhance the increase of the coupling matrix elements through the vibronic coupling between the excited singlet states. The remarkable rotational quantum species dependence on the ISC rate constant (kISC) value clearly appeared in m-MA. The dependence should result from the difference of the ρ value between a1 and e species, since the e species are doubly degenerate. The species dependence was apparently related to the potential barrier height, suggesting that the large barrier height should have an influence on the ρ value of the triplet states.
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