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On the vibronic level structure in the NO3 radical. I. The ground electronic statel

机译:在NO3自由基的电子振动能级结构上。在。地面电子状态

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The model Hamiltonian approach of Koppel [Adv. Chem. Phys. 57, 59 (1984)] is used to analyze the electronic spectroscopy of the nitrate radical (NO3). Simulations of negative ion photodetachment of NO3-, the X (2)A(2)(')<- B E-2(') dispersed fluorescence spectrum of NO3, and the B E-2(')<- X (2)A(2)(') absorption spectrum are all in qualitative agreement with experiment, indicating that the model Hamiltonian contains most or all of the essential physics that govern the strongly coupled X (2)A(2)(') and B E-2(') electronic states of the radical. All 14 bands seen in the dispersed fluorescence spectrum below 2600 cm(-1) are assigned based on the simulations, filling in a few gaps left by previous work, and 7 additional bands below 4000 cm(-1) are tentatively assigned. The assignment is predicated on the assumption that the nu(3) level of NO3 is near 1000 cm(-1) rather than 1492 cm(-1) as is presently believed. Support for this reassignment (which associates the 1492 cm(-1) band with the nu(1)+nu(4) level) comes from both the model Hamiltonian spectrum and a Fourier-transform infrared feature at 2585 cm(-1) that is consistent with the large and positive cross anharmonicity between nu(1) and nu(4) needed for the alternative 1492 cm(-1) assignment. An apparent systematic deficiency exists in the treatment of the model Hamiltonian for levels involving nu(4). A discussion of the correlation between energy levels in the rigid D-3h and C-2v limits is illustrative, and provides insight into just how hard it is to treat the degenerate bending coordinate (q(4)) of NO3 accurately. (c) 2007 American Institute of Physics.
机译:Koppel的模型哈密顿方法[Adv。化学物理57,59(1984)]用于分析硝酸根(NO3)的电子光谱。 NO3-,X(2)A(2)(')<-B E-2(')分散的NO3的荧光光谱和B E-2(')<-X(2 )A(2)(')吸收光谱都与实验定性一致,表明哈密顿量模型包含控制强耦合X(2)A(2)(')和B E的大部分或全部基本物理。 -2(')自由基的电子态。根据模拟结果,分配了在2600 cm(-1)以下的分散荧光光谱中看到的所有14条带,填补了先前工作留下的一些空白,并尝试分配了4000 cm(-1)以下的另外7条带。该分配基于以下假设:NO3的nu(3)水平接近1000 cm(-1),而不是目前认为的1492 cm(-1)。支持此重新分配(将1492 cm(-1)波段与nu(1)+ nu(4)级别相关联)来自模型哈密顿光谱和2585 cm(-1)处的傅立叶变换红外特征与替代1492 cm(-1)分配所需的nu(1)和nu(4)之间的较大且正的交叉非谐性一致。在涉及nu(4)的水平的模型哈密顿量的处理中存在明显的系统缺陷。对刚性D-3h和C-2v极限中的能级之间的相关性的讨论是说明性的,并提供了深入了解准确处理NO3的简并弯曲坐标(q(4))的难度。 (c)2007年美国物理研究所。

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