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来自……的光化学自由基形成的超快动力学

Ultrafast dynamics of photochemical radical formation from.

作者信息

Farrell IR, Matousek P, Kleverlaan CJ, Vlcek A

机构信息

Department of Chemistry, Queen Mary and Westfield College (University of London), UK.

出版信息

Chemistry. 2000 Apr 14;6(8):1386-94. doi: 10.1002/(sici)1521-3765(20000417)6:8<1386::aid-chem1386>3.0.co;2-g.

Abstract

The excited-state dynamics and photochemistry of [Re(R)(CO)3(dmb)] (R=Me, Et); dmb=4,4'-dimethyl-2,2'-bipyridine) in CH2Cl2 have been studied by time-resolved visible absorption spectroscopy on a broad time scale ranging from approximately 400 fs to a few microseconds, with emphasis on the femtosecond and picosecond dynamics. It was found that the optically prepared Franck-Condon 1MLCT (singlet metal-to-ligand charge transfer) excited state of [Re(R)(CO)3(dmb)] undergoes femtosecond branching between two pathways (< or =400 fs for R=Me; approximately 800 fs for R=Et). For both methyl and ethyl complexes, evolution along one pathway leads to homolysis of the Re-R bond via a 3SBLCT (triplet sigma-bond-to-ligand charge transfer) excited state, from which [Re(S)(CO)3(dmb)]* and R* radicals are formed. The other pathway leads to an inherently unreactive 3MLCT state. For [Re(Me)(CO)3(dmb)], the 3MLCT state lies lowest in energy and decays exclusively to the ground state with a lifetime of approximately 35 ns, thereby acting as an excitation energy trap. The reactive 3SBLCT state is higher in energy. The quantum yield (0.4 at 293 K) of the radical formation is determined by the branching ratio between the two pathways. [Re(Et)(CO)3(dmb)] behaves differently: branching of the Franck-Condon state between two pathways still occurs, but the 3MLCT excited state lies above the dissociative 3SBLCT state and can decay into it. This shortens the 3MLCT lifetime to 213 ps in CH2Cl2 or 83 ps in CH3CN. Once populated, the 3SBLCT state evolves toward radical photoproducts [Re(S)(CO)3(dmb)]* and Et*. Thus, population of the 3MLCT excited state of [Re(Et)(CO)3(dmb)] provides a second, delayed pathway to homolysis. Hence, the quantum yield is unity. The photochemistry and excited-state dynamics of [Re(R)(CO)3(dmb)] (R=Me, Et) complexes are explained in terms of the relative ordering of the Franck-Condon, 3MLCT, and 3SBLCT states in the region of vertical excitation and along the Re-R reaction coordinate. A qualitative potential energy diagram is proposed.

摘要

通过时间分辨可见吸收光谱,在大约400飞秒到几微秒的宽时间尺度上,重点研究了[Re(R)(CO)₃(dmb)](R = Me,Et;dmb = 4,4'-二甲基-2,2'-联吡啶)在二氯甲烷中的激发态动力学和光化学,特别关注飞秒和皮秒动力学。研究发现,[Re(R)(CO)₃(dmb)]光学制备的弗兰克 - 康登1MLCT(单线态金属到配体电荷转移)激发态在两条路径之间发生飞秒级分支(R = Me时≤400飞秒;R = Et时约800飞秒)。对于甲基和乙基配合物,沿一条路径的演化通过3SBLCT(三线态σ键到配体电荷转移)激发态导致Re - R键的均裂,从中形成[Re(S)(CO)₃(dmb)]和R自由基。另一条路径导致本质上无反应性的3MLCT态。对于[Re(Me)(CO)₃(dmb)],3MLCT态能量最低,仅以约35纳秒的寿命衰减到基态,因此起到激发能陷阱的作用。反应性的3SBLCT态能量更高。自由基形成的量子产率(293 K时为0.4)由两条路径之间的分支比决定。[Re(Et)(CO)₃(dmb)]的行为不同:弗兰克 - 康登态在两条路径之间的分支仍然发生,但3MLCT激发态高于解离性的3SBLCT态,并且可以衰变为该态。这将3MLCT寿命缩短至二氯甲烷中为213皮秒或乙腈中为83皮秒。一旦形成,3SBLCT态向自由基光产物[Re(S)(CO)₃(dmb)]和Et演化。因此,[Re(Et)(CO)₃(dmb)]的3MLCT激发态的形成提供了第二条延迟的均裂路径。因此,量子产率为1。[Re(R)(CO)₃(dmb)](R = Me,Et)配合物的光化学和激发态动力学是根据垂直激发区域以及沿Re - R反应坐标的弗兰克 - 康登、3MLCT和3SBLCT态的相对排序来解释的。提出了一个定性势能图。

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