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飞秒时间尺度下近紫外光谱区激发吡咯分子的演化。

Femtosecond evolution of the pyrrole molecule excited in the near part of its UV spectrum.

机构信息

Departamento de Química Física, Universidad del País Vasco (UPV∕EHU), Apart. 644, 48080 Bilbao, Spain.

出版信息

J Chem Phys. 2012 Aug 14;137(6):064317. doi: 10.1063/1.4742344.

DOI:10.1063/1.4742344
PMID:22897283
Abstract

The evolution of the isolated pyrrole molecule has been followed after excitation in the 265-217 nm range by using femtosecond time delayed ionization. The transients collected in the whole excitation range show the vanishing of the ionization signal in the femtosecond time scale, caused by the relaxation along a πσ(∗) type state (3s a(1)←π 1a(2)), which is the lowest excited electronic state of the molecule. This surface is dissociative along the NH bond, yielding a 15 ± 3 fs lifetime that reflects the loss of the ionization cross-section induced by the ultrafast wavepacket motion. Although a weak πσ(∗) absorption is detected, the state is mainly reached through internal conversion of the higher bright ππ(∗) transitions, which occurs with a 19 ± 3 fs lifetime. In addition to its resonant excitation, the intense ππ(∗) absorption extending in the 220-190 nm interval is also out-of-resonance populated at energies far to the red from its absorption onset. This coherent adiabatic excitation of the ππ(∗) transition should follow the excitation pulse (coherent population return effect), but instead the system relaxes toward the lower πσ(∗) surface through a conical intersection during the interaction time, leading to the population of πσ(∗) state at wavelengths as long as 265 nm. According to the observed behavior, the time evolution of the system in the full excitation range studied is modeled by a coherent treatment that provides key insights on the photophysical properties of the molecule.

摘要

孤立吡咯分子在 265-217nm 范围内被激发后,通过使用飞秒时间延迟电离,对其激发态的演化进行了跟踪。在整个激发范围内收集的瞬态信号显示,在飞秒时间尺度上,由于沿着 πσ()(3sa(1)←π1a(2))类型态的弛豫,导致电离信号消失,该态是分子的最低激发电子态。这个表面沿着 NH 键离解,产生 15±3fs 的寿命,反映了由超快波包运动引起的电离截面的损失。尽管检测到较弱的 πσ()吸收,但该态主要通过较高的明亮 ππ()跃迁的内部转换到达,其寿命为 19±3fs。除了共振激发之外,在 220-190nm 间隔内延伸的强烈 ππ()吸收也在远离其吸收起始能量的远红光区以非共振方式被激发。这种 ππ()跃迁的相干绝热激发应该跟随激发脉冲(相干布居返驰效应),但在相互作用时间内,系统通过锥形交叉点向较低的 πσ()表面弛豫,导致在长达 265nm 的波长处激发态πσ(*). 根据观察到的行为,用相干处理方法对系统在整个激发范围内的时间演化进行了建模,该方法为分子的光物理性质提供了关键的见解。

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