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推拉型偶氮苯染料-半导体复合物中电荷转移驱动的结构弛豫

Charge Transfer Driven Structural Relaxation in a Push-Pull Azobenzene Dye-Semiconductor Complex.

作者信息

Torres Alberto, Prado Luciano R, Bortolini Graziele, Rego Luis G C

机构信息

Department of Physics , Universidade Federal de Santa Catarina , Florianópolis , SC 88040-900 , Brazil.

出版信息

J Phys Chem Lett. 2018 Oct 18;9(20):5926-5933. doi: 10.1021/acs.jpclett.8b02490. Epub 2018 Sep 28.

Abstract

Photoexcited structural dynamics in azo-compounds may differ fundamentally whether the push-pull photochromic azo-compound is isolated or forms a heterogeneous charge transfer complex, due to a sudden oxidation of the chromophore. Herein, we use a quantum-classical self-consistent approach that incorporates nonadiabatic excited-state electronic quantum dynamics into molecular mechanics to study the photoexcited dynamics of the push-pull azo-compound para-Methyl Red in the gas phase and sensitizing the (101) anatase surface of TiO. We find that the photoinduced S/S trans-to- cis isomerization of para-Methyl Red in the gas phase occurs through a pedal-like torsion around the ϕ dihedral angle, without evidence to support the inversion mechanism, likewise in the parent azobenzene molecule. However, the photoexcited structural relaxation of the charge transfer complex para-Methyl Red/TiO contrasts essentially with the isolated azo-compounds. Immediately after photoexcitation, the excited electron flows into the TiO conduction band, with an injection time constant of ≃5 fs, and no indication of isomerization is observed during the 1.5 ps simulations. Instead, a strong vibronic relaxation occurs that excites the NN stretching mode of the azo-group, which is ultimately ascribed to the NA relaxation, and delocalization, of the hole wavepacket.

摘要

由于发色团的突然氧化,推拉光致变色偶氮化合物在孤立状态或形成异质电荷转移络合物时,其光激发结构动力学可能存在根本差异。在此,我们采用一种量子-经典自洽方法,该方法将非绝热激发态电子量子动力学纳入分子力学,以研究推拉偶氮化合物对甲基红在气相中的光激发动力学以及对TiO(101)锐钛矿表面的敏化作用。我们发现,气相中对甲基红的光致S/S反式-顺式异构化是通过围绕ϕ二面角的踏板状扭转发生的,没有证据支持反转机制,这与母体偶氮苯分子情况相同。然而,电荷转移络合物对甲基红/TiO的光激发结构弛豫与孤立的偶氮化合物基本不同。光激发后,激发电子立即流入TiO导带,注入时间常数约为5 fs,在1.5 ps模拟过程中未观察到异构化迹象。相反,发生了强烈的振动弛豫,激发了偶氮基团的NN伸缩模式,这最终归因于空穴波包的NA弛豫和离域。

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