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在紫外区域光解后,乙二醛通过S0和T1途径产生的碎片HCO的内部状态分布。

Internal state distributions of fragment HCO via S0 and T1 pathways of glyoxal after photolysis in the ultraviolet region.

作者信息

Kao Chih Chieh, Ho Mei-Lin, Chen Ming-Wei, Lee Sheng-Jui, Chen I-Chia

机构信息

Department of Chemistry, National Tsing Hua University, Hsinchu, Taiwan 30013, Republic of China.

出版信息

J Chem Phys. 2004 Mar 15;120(11):5087-95. doi: 10.1063/1.1647538.

Abstract

The dynamics of photodissociation of glyoxal (HOC-COH) near the dissociation threshold on the triplet manifold are studied through measurement of distributions of nascent fragment HCO in various internal states. Three rotational levels 1(01) (), 4(13) (), and 3(21) ()+3(22) () of vibrational state U (excitation wavelength approximately 394.4 nm, origin at 25,331.865 cm(-1)) of glyoxal in state A (1)A(u) and two other vibrational states at excitation wavelengths 390.33 and 382.65 nm are selected to produce fragment HCO. By means of fluorescence in the transition B (2)A(')-X (2)A(') of HCO, we determined the relative populations of internal states of that fragment. Rotational states of product HCO up to N=26 and K=2 are populated, and bimodal distributions of these rotational states are observed for the photolysis wavelengths used in this work. The high rotational part of the distribution with average energy near values calculated on the basis of the statistical model-phase-space theory is assigned to arise from glyoxal on its S(0) surface, and the low rotational part from the T(1) surface with an exit barrier. After photolysis near the threshold region on the triplet surface, HCO arising from the T(1) state appears to be a major component of products because these rotational levels 1(01) (), 4(13) (), and 3(2) (*) of U state selected are gateway states with an enhanced rate of intersystem crossing.

摘要

通过测量新生碎片 HCO 在各种内部状态下的分布,研究了乙二醛(HOC - COH)在三重态流形上离解阈值附近的光解动力学。选择处于 A(1)A(u) 态的乙二醛的振动状态 U(激发波长约为 394.4 nm,起始于 25,331.865 cm⁻¹)的三个转动能级 1(01) ()、4(13) () 和 3(21) ()+3(22) (),以及在激发波长 390.33 和 382.65 nm 下的另外两个振动状态来产生碎片 HCO。借助 HCO 在 B(2)A(')-X(2)A(') 跃迁中的荧光,我们确定了该碎片内部状态的相对布居数。产物 HCO 的转动状态填充到 N = 26 和 K = 2,并且在本工作中使用的光解波长下观察到这些转动状态的双峰分布。分布中平均能量接近基于统计模型 - 相空间理论计算值的高转动部分被认为是由处于 S(0) 表面的乙二醛产生的,而低转动部分则来自具有出射势垒的 T(1) 表面。在三重态表面的阈值区域附近进行光解后,来自 T(1) 态的 HCO 似乎是产物的主要成分,因为所选择的 U 态的这些转动能级 1(01) ()、4(13) () 和 3(2) (*) 是具有增强的系间窜越速率的通道态。

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