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通过超声速射流膨胀束中的激光双共振方法确定的CdAr络合物最低电子里德堡态的结构。

The structure of the lowest electronic Rydberg state of CdAr complex determined by laser double resonance method in a supersonic jet-expansion beam.

作者信息

Koperski J, Czajkowski M

机构信息

Instytut Fizyki, Uniwersytet Jagielloński, ul. Reymonta 4, 30-059 Kraków, Poland.

出版信息

Spectrochim Acta A Mol Biomol Spectrosc. 2003 Sep;59(11):2435-48. doi: 10.1016/s1386-1425(02)00396-7.

DOI:10.1016/s1386-1425(02)00396-7
PMID:12963441
Abstract

The lowest E1(3Sigma(+)) Rydberg state of the CdAr van der Waals (vdW) complex was investigated by means of an optical-optical double resonance (OODR) method of laser spectroscopy in conjunction with a free jet-expansion molecular beam. Two dye lasers were employed for the two-step excitation. The A0(+)(3Pi(+)) and B1(3Sigma(+)) states were used as intermediates in the excitation process from the X0(+)(1Sigma(+)) ground state. Two types of bound-bound excitation spectra of the E1<--A0(+) and E1<--B1 transitions were recorded indicating the existence of two, well defined minima in the E1-state potential energy (PE) curve. First, considerably deep, with the well depth of D(e)'(E1(2))=1309.0 cm(-1) and second, separated by a positive PE barrier, with D(e)'(E1(2))=24.2 cm(-1). Combination of bound-bound and first-time observed bound-free excitation spectra enabled a complete determination of the spectroscopical parameters of the PE curve of the E1-Rydberg state, the height of the PE barrier and its approximate location. In the excitation spectra of the E1<--B1 transition, a nodal structure of the bound-free transitions was observed and elucidated by a projection of the B1-state vibrational wave-functions onto the E1-state potential barrier and/or onto the repulsive part of the E1-state PE curve. The experimental results of our investigation coincides well with recently published results of ab initio calculation of Czuchaj and co-workers [Chem. Phys. 248 (1999) 1; Chem Phys. 263 (2001) 7; Theor. Chem Acc. 105 (2001) 219].

摘要

通过激光光谱的光学-光学双共振(OODR)方法结合自由射流膨胀分子束,对CdAr范德华(vdW)复合物的最低E1(3Σ(+)) 里德堡态进行了研究。使用两台染料激光器进行两步激发。在从X0(+)(1Σ(+))基态的激发过程中,A0(+)(3Π(+))和B1(3Σ(+))态被用作中间态。记录了E1<--A0(+)和E1<--B1跃迁的两种类型的束缚-束缚激发光谱,表明在E1态势能(PE)曲线中存在两个明确的极小值。首先,相当深,阱深D(e)'(E1(2)) = 1309.0 cm(-1),其次,被一个正的PE势垒隔开,D(e)'(E1(2)) = 24.2 cm(-1)。束缚-束缚和首次观测到的束缚-自由激发光谱的结合,使得能够完整地确定E1-里德堡态PE曲线的光谱参数、PE势垒的高度及其大致位置。在E1<--B1跃迁的激发光谱中,观察到了束缚-自由跃迁的节点结构,并通过将B1态振动波函数投影到E1态势垒和/或E1态PE曲线的排斥部分来进行解释。我们的研究实验结果与Czuchaj及其同事最近发表的从头算结果[《化学物理》248 (1999) 1;《化学物理》263 (2001) 7;《理论化学学报》105 (2001) 2,19]非常吻合。

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