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RESONANCE ENHANCED MULTIPHOTON IONIZATION SPECTROSCOPY OF CARBON DISULPHIDE

机译:二硫化碳的共振增强多光子电离光谱

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Rydberg excited states of the CS2 molecule in the energy range 56 000-81 000 cm(-1) have been further investigated via the two and three photon resonance enhancements they provide in the mass resolved multiphoton ionization (MPI) spectrum of a jet-cooled sample of a parent molecule. Spectral interpretation has been aided by parallel measurements of the kinetic energies of the photoelectrons that accompany the various MPI resonances. Thus we have been able to extend, and clarify, previous analyses of the tangled spin-orbit split vibronic structure associated with the (IIu)-I-3 and (IIu)-I-1 states derived from the configuration [(IIg)-I-2]4p sigma(u) and the (3) Delta(u), (1) Delta(u), and (1) Sigma(u)(+) states resulting from the configuration [(IIg)-I-2]4p pi(u), and to deduce an approximate wave number for the origin of the hitherto unidentified (3) Sigma(u)(+) state derived from this same configuration. Moving to higher energies we are able to locate, unambiguously, the origins of the next (n=5) members of four of these [(IIg)-I-2]np Rydberg series, and to identify extensive series based on the presumed Rydberg configurations [(IIg)-I-2]ns sigma(g) and [(IIg)-I-2]nf lambda(u) with, in both cases, n less than or equal to 10. We also identify MPI resonances attributable to CS(a(3)II) fragments, to ground state C atoms, and to S atoms in both their ground (P-3) and excited (S-1) electronic states. Analysis of the former resonances indicates that the CS(a(3)II) fragments resulting from two photon dissociation of CS2 at excitation wavelengths around 300 nm are formed with substantial rovibrational excitation. (C) 1996 American Institute of Physics. [References: 63]
机译:通过在喷气冷却的质量分辨多光子电离(MPI)光谱中提供的两个和三个光子共振增强,进一步研究了CS2分子在56 000-81 000 cm(-1)能量范围内的Rydberg激发态母体分子的样品。通过并行测量伴随各种MPI共振的光电子动能,有助于光谱解释。因此,我们已经能够扩展和阐明以前与自构型[[(IIg)-]衍生的(IIu)-I-3和(IIu)-I-1状态相关的自旋轨道分裂振动电子结构的先前分析。 I-2] 4p sigma(u)和(3)Delta(u),(1)Delta(u)和(1)Sigma(u)(+)状态由[[IIg)-I- 2] 4p pi(u),并推论出从相同配置导出的迄今未确定的(3)Sigma(u)(+)状态起源的近似波数。转向更高的能量,我们能够毫无疑问地找到这些[(IIg)-I-2] np Rydberg系列中的四个(n = 5)成员的起源,并根据假定的Rydberg来确定广泛的系列构型[(IIg)-I-2] ns sigma(g)和[(IIg)-I-2] nf lambda(u),在两种情况下,n均小于或等于10。我们还确定了MPI共振可归因于CS(a(3)II)碎片,基态C原子和S原子处于基态(P-3)和激发态(S-1)。对前者共振的分析表明,由CS2的两个光子在300 nm左右的激发波长处解离产生的CS(a(3)II)片段是通过大量振动激发形成的。 (C)1996年美国物理研究所。 [参考:63]

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