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硝萘衍生物的激发态动力学:在数百飞秒内发生系间窜跃至三重态能级。

Excited-state dynamics in nitro-naphthalene derivatives: intersystem crossing to the triplet manifold in hundreds of femtoseconds.

机构信息

Department of Chemistry, Center for Chemical Dynamics, Case Western Reserve University, 10900 Euclid Avenue, Cleveland, Ohio 44106, United States.

出版信息

J Phys Chem A. 2013 Aug 1;117(30):6580-8. doi: 10.1021/jp405656n. Epub 2013 Jul 11.

Abstract

Femtosecond transient absorption experiments and density functional calculations are presented for 2-methyl-1-nitronaphthalene, 2-nitronaphthalene, and 1-nitronaphthalene in cyclohexane and acetonitrile solutions. Excitation of 2-methyl-1-nitronaphthalene at 340 nm populates the Franck-Condon singlet state, which bifurcates into two barrierless decay channels with sub-200-fs lifetimes. The primary decay channel connects the Franck-Condon singlet excited state with a receiver triplet state, whereas the second, minor channel involves conformational relaxation to populate an intramolecular charge-transfer state, as previously reported for 1-nitronaphthalene (J. Chem. Phys. 2009, 113, 224518). Conversely, the experimental and computational data for 2-nitronaphthalene shows that almost the entire Franck-Condon singlet excited-state population intersystem crosses to the triplet state in less than 200 fs due to a sizable energy barrier of ca. 5 kcal/mol that must be surmounted to access the intramolecular charge-transfer state. Our results lend support to the idea that the probability of population transfer to the triplet manifold in these nitronaphthalene derivatives is controlled not only by the small energy gap between the Franck-Condon singlet excited state and the receiver triplet state but also by the region of configuration space sampled in the singlet excited-state potential energy surface at the time of excitation. It is proposed that the ultrafast intersystem crossing dynamics in these nitronaphthalene molecules most likely occurs between nonequilibrated excited states in the strongly nonadiabatic regime.

摘要

飞秒瞬态吸收实验和密度泛函计算被应用于 2-甲基-1-硝基萘、2-硝基萘和 1-硝基萘在环己烷和乙腈溶液中的研究。340nm 激发 2-甲基-1-硝基萘,生成 Franck-Condon 单重激发态,该激发态通过两个无势垒的衰减通道进行衰减,其衰减寿命小于 200fs。主要的衰减通道将 Franck-Condon 单重激发态与受体三重态连接,而第二个次要通道涉及构象松弛,以填充分子内电荷转移态,这与之前对 1-硝基萘的研究结果一致(J. Chem. Phys. 2009, 113, 224518)。相反,2-硝基萘的实验和计算数据表明,由于约 5kcal/mol 的大能量势垒,几乎整个 Franck-Condon 单重激发态的电子在 200fs 内通过系间窜越转移到三重态,该能量势垒必须被克服才能到达分子内电荷转移态。我们的结果支持了这样的观点,即在这些硝基萘衍生物中,电子转移到三重态的概率不仅由 Franck-Condon 单重激发态和受体三重态之间的小能隙控制,而且还由激发时单重激发态势能面中构型空间的区域控制。我们提出,这些硝基萘分子中超快的系间窜越动力学最有可能发生在强非绝热区域中未平衡的激发态之间。

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