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通过速度成像研究 N-亚硝基吡咯烷从第一和第二激发单线态的光解动力学。

The photodissociation dynamics of N-nitrosopyrrolidine from the first and second excited singlet states studied by velocity map imaging.

机构信息

Institut für Physikalische und Theoretische Chemie, Universität Regensburg, 93053 Regensburg, Germany.

出版信息

Phys Chem Chem Phys. 2010 May 14;12(18):4644-55. doi: 10.1039/b920547k. Epub 2010 Jan 28.

DOI:10.1039/b920547k
PMID:20428544
Abstract

The photodissociation reaction of N-nitrosopyrrolidine isolated and cooled in a supersonic jet has been studied following excitation to the S(1) and S(2) electronic states. The nascent NO (X[combining tilde] (2)Pi((1/2),3/2), v, j) radicals were ionized by state-selective (1 + 1)-REMPI via the A(2)Sigma(+) state. The angularly resolved velocity distribution of these ions was measured with the velocity-map imaging (VMI) technique. Photodissociation from S(1) produces NO in the vibrational ground state and the pyrrolidine radical in the electronic ground state 1 (2)B. About 73% of the excess energy is converted into kinetic energy of the fragments. The velocity distribution shows a strong negative anisotropy (beta = -0.9) in accordance with the npi*-character of the S(0)--> S(1) transition. An upper limit for the N-NO dissociation energy of (14 640 +/- 340) cm(-1) is determined. We conclude that photodissociation from S(1) occurs very fast on a completely repulsive potential energy surface. Excitation into the S(2)pipi*-state leads to a bimodal velocity distribution. Two dissociation channels can be distinguished which show both positive anisotropy (beta = 1.3 and 1.6) but differ considerably in the total kinetic energy and the rotational energy of the NO fragment. We assign one channel to the direct dissociation on the S(2) potential energy surface, leading to pyrrolidine radicals in the excited electronic state 1 (2)A. The second channel leads to pyrrolidine in the electronic ground state 1 (2)B, presumably after crossing to the S(1) state via a conical intersection.

摘要

已在超音速射流中进行了氮-亚硝基吡咯烷的光解反应的研究,其激发到 S(1) 和 S(2) 电子态。初生的 NO (X[combining tilde] (2)Pi((1/2),3/2), v, j) 自由基通过状态选择性 (1 + 1)-REMPI 通过 A(2)Sigma(+) 态被离子化。这些离子的角分辨速度分布通过速度映射成像 (VMI) 技术进行测量。S(1) 光解产生振动基态的 NO 和电子基态 1 (2)B 的吡咯烷自由基。大约 73%的过剩能量转化为碎片的动能。速度分布显示出强烈的负各向异性 (β=-0.9),与 S(0)-->S(1) 跃迁的 npi*-特征一致。确定 N-NO 离解能的上限为 (14640 ± 340) cm(-1)。我们得出结论,S(1) 光解在完全排斥的势能表面上发生得非常快。激发到 S(2)pipi*-态导致双峰速度分布。可以区分两个离解通道,它们都显示出正各向异性 (β=1.3 和 1.6),但总动能和 NO 碎片的转动能差异很大。我们将一个通道归因于 S(2)势能表面上的直接离解,导致吡咯烷自由基处于激发的电子态 1 (2)A。第二个通道导致吡咯烷处于电子基态 1 (2)B,可能是通过锥形交叉点先跃迁到 S(1)态后再发生的。

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