TY - JOUR
T1 - Different photoisomerization routes found in the structural isomers of hydroxy methylcinnamate
AU - Kinoshita, Shin Nosuke
AU - Miyazaki, Yasunori
AU - Sumida, Masataka
AU - Onitsuka, Yuuki
AU - Kohguchi, Hiroshi
AU - Inokuchi, Yoshiya
AU - Akai, Nobuyuki
AU - Shiraogawa, Takafumi
AU - Ehara, Masahiro
AU - Yamazaki, Kaoru
AU - Harabuchi, Yu
AU - Maeda, Satoshi
AU - Taketsugu, Tetsuya
AU - Ebata, Takayuki
N1 - Funding Information:
Y. I., M. E., and H. K. acknowledge Grants-in-Aid for Scientific Research (KAKENHI) by the Ministry of Education, Culture, Sports, Science and Technology (MEXT) No. 25410017, 16H04098, 16H04104, and 15KT0065, respectively. S. M., T. T., K. Y., and Y. H. acknowledge a grant from the Japan Science and Technology Agency (JST) with Core Research for Evolutional Science and Technology (CREST, grant number JPMJCR14L5) in the Area of ‘‘Establishment of Molecular Technology towards the Creation of New Functions’’ at Hokkaido University. K. Y. is grateful for the financial support from Building of Consortia for the Development of Human Resources in Science and Technology, MEXT. Y. H. acknowledges the financial support from JST, PREST (grant number JPMJPR16N8). T. E. acknowledges the financial support from the Institute for Quantum Chemical Exploration. This work was also partially supported by the Joint Studies Program (2014–2016) of IMS. Part of the calculations in this paper was carried out by using the supercomputers at Academic Center for Computing and Media Studies, Kyoto University and Okazaki Research Facilities (Research Center for Computational Science).
Publisher Copyright:
© the Owner Societies.
PY - 2018
Y1 - 2018
N2 - An experimental and theoretical study has been carried out to elucidate the nonradiative decay (NRD) and trans(E) → cis(Z) isomerization from the S1 (1ππ∗) state of structural isomers of hydroxy methylcinnamate (HMC); ortho-, meta- and para-HMC (o-, m- and p-HMC). A low temperature matrix-isolation Fourier Transform Infrared (FTIR) spectroscopic study revealed that all the HMCs are cis-isomerized upon UV irradiation. A variety of laser spectroscopic methods have been utilized for jet-cooled gas phase molecules to investigate the vibronic structure and lifetimes of the S1 state, and to detect the transient state appearing in the NRD process. In p-HMC, the zero-point level of the S1 state decays as quickly as 9 ps. A transient electronic state reported by Tan et al. (Faraday Discuss. 2013, 163, 321-340) was reinvestigated by nanosecond UV-tunable deep UV pump-probe spectroscopy and was assigned to the T1 state. For m- and o-HMC, the lifetime at the zero-point energy level of S1 is 10 ns and 6 ns, respectively, but it becomes substantially shorter at an excess energy higher than 1000 cm-1 and 600 cm-1, respectively, indicating the onset of NRD. Different from p-HMC, no transient state (T1) was observed in m- nor o-HMC. These experimental results are interpreted with the aid of TDDFT calculations by considering the excited-state reaction pathways and the radiative/nonradiative rate constants. It is concluded that in p-HMC, the trans → cis isomerization proceeds via a [trans-S1 → 1nπ∗ → T1 → cis-S0] scheme. On the other hand, in o- and m-HMC, the isomerization proceeds via a [trans-S1 → twisting along the CC double bond by 90° on S1 → cis-S0] scheme. The calculated barrier height along the twisting coordinate agrees well with the observed onset of the NRD channel for both o- and m-HMC.
AB - An experimental and theoretical study has been carried out to elucidate the nonradiative decay (NRD) and trans(E) → cis(Z) isomerization from the S1 (1ππ∗) state of structural isomers of hydroxy methylcinnamate (HMC); ortho-, meta- and para-HMC (o-, m- and p-HMC). A low temperature matrix-isolation Fourier Transform Infrared (FTIR) spectroscopic study revealed that all the HMCs are cis-isomerized upon UV irradiation. A variety of laser spectroscopic methods have been utilized for jet-cooled gas phase molecules to investigate the vibronic structure and lifetimes of the S1 state, and to detect the transient state appearing in the NRD process. In p-HMC, the zero-point level of the S1 state decays as quickly as 9 ps. A transient electronic state reported by Tan et al. (Faraday Discuss. 2013, 163, 321-340) was reinvestigated by nanosecond UV-tunable deep UV pump-probe spectroscopy and was assigned to the T1 state. For m- and o-HMC, the lifetime at the zero-point energy level of S1 is 10 ns and 6 ns, respectively, but it becomes substantially shorter at an excess energy higher than 1000 cm-1 and 600 cm-1, respectively, indicating the onset of NRD. Different from p-HMC, no transient state (T1) was observed in m- nor o-HMC. These experimental results are interpreted with the aid of TDDFT calculations by considering the excited-state reaction pathways and the radiative/nonradiative rate constants. It is concluded that in p-HMC, the trans → cis isomerization proceeds via a [trans-S1 → 1nπ∗ → T1 → cis-S0] scheme. On the other hand, in o- and m-HMC, the isomerization proceeds via a [trans-S1 → twisting along the CC double bond by 90° on S1 → cis-S0] scheme. The calculated barrier height along the twisting coordinate agrees well with the observed onset of the NRD channel for both o- and m-HMC.
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U2 - 10.1039/c8cp00414e
DO - 10.1039/c8cp00414e
M3 - Article
C2 - 29693100
AN - SCOPUS:85049652462
VL - 20
SP - 17583
EP - 17598
JO - Physical Chemistry Chemical Physics
JF - Physical Chemistry Chemical Physics
SN - 1463-9076
IS - 26
ER -