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首页> 外文期刊>The Journal of Chemical Physics >A DEPERTURBATION ANALYSIS OF THE B-3-SIGMA(-)(U)(V'=0-6) AND THE B''(3)PI(U)(V'=2-12) STATES OF S-2
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A DEPERTURBATION ANALYSIS OF THE B-3-SIGMA(-)(U)(V'=0-6) AND THE B''(3)PI(U)(V'=2-12) STATES OF S-2

机译:S-3的B-3-SIGMA(-)(U)(V'= 0-6)和B''(3)PI(U)(V'= 2-12)状态的去扰动分析

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Laser-induced fluorescence spectra of S-32(2) have been obtained, covering upsilon'=0-6 of the B (3) Sigma(u)(-)-X (3) Sigma(g)(-) transition and upsilon'=2-12 of the B ''(3) Pi(u)-X(3) Sigma(g)(-) transition, using static cell and supersonic free jet techniques. The spectra include transitions to the previously unseen B ''(3) Pi(2,u) components. Analysis of the many perturbations between the two upper electronic states has been carried out using a Hamiltonian matrix including- all the B and B '' states simultaneously rather than deperturbing individual pairs of vibronic states. This takes into account longer range interactions and gives deperturbed molecular constants that vary smoothly with vibrational state. Our model for the B ''upsilon'=2-12 and B upsilon'=0-6 levels covering J up to 100 can fit all 3320 observed transitions with an average error of 0.064 cm(-1). The widely ranging fluorescence lifetimes of the B '' state vibronic levels provide independent information about thr state mixing and confirm the model, since the observed B ''-X fluorescence arises-almost entirely via this mixing. However, lifetime measurements of the newly observed Omega=2 components of the B '' state showed little variation in lifetimes, about an average of 4.2+/-0.4 mu s. This indicates a small intrinsic B ''-X transition strength as the Omega=2 components are essentially not mixed with the B state. A model for the perturbation parameters is developed,- based on Franck-Condon-factors between the two states. The magnitude of the perturbations and transition moments are discussed in relation to the electronic configurations of the B and B '' states. (C) 1996 American Institute of Physics. [References: 38]
机译:已经获得了S-32(2)的激光诱导荧光光谱,涵盖了B(3)Sigma(u)(-)-X(3)Sigma(g)(-)跃迁和使用静态单元格和超音速自由射流技术,使B''(3)Pi(u)-X(3)Sigma(g)(-)跃迁的upsilon'= 2-12。光谱包括到以前看不见的B''(3)Pi(2,u)组分的跃迁。已经使用包含所有B和B''状态的哈密顿矩阵对两个上部电子状态之间的许多扰动进行了分析,而不是对单个的振动状态进行扰动。这考虑到了更长距离的相互作用,并给出了受扰动的分子常数,该常数随振动状态而平稳变化。我们的模型B'upsilon'= 2-12和B upsilon'= 0-6覆盖了100个J,可以拟合所有3320个观测到的跃迁,平均误差为0.064 cm(-1)。由于观察到的B''-X荧光几乎全部是通过这种混合产生的,因此B''状态振动子的荧光寿命范围广泛,可提供有关thr状态混合的独立信息并确认模型。但是,对新观察到的B”状态的Omega = 2成分的寿命测量显示寿命几乎没有变化,平均约为4.2 +/- 0.4μs。这表明由于Omega = 2组分基本上不与B状态混合,因此固有的B''-X过渡强度很小。基于两种状态之间的弗兰克-康登因子,开发了一种扰动参数模型。关于B和B''状态的电子结构,讨论了扰动和跃迁的大小。 (C)1996年美国物理研究所。 [参考:38]

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