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首页> 外文期刊>The Journal of Chemical Physics >Molecular-beam infrared-infrared double-resonance spectroscopy study of the vibrational dynamics of the acetylenic C-H stretch of propargyl amine
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Molecular-beam infrared-infrared double-resonance spectroscopy study of the vibrational dynamics of the acetylenic C-H stretch of propargyl amine

机译:炔丙胺炔属C-H链段振动动力学的分子束红外-红外双共振光谱研究

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摘要

The acetylenic C-H stretch spectrum of propargyl amine near 3330 cm(-1) has been measured at 0.0002 cm(-1) (6 MHz) resolution with a tunable color-center laser in an electric-resonance optothermal spectrometer. The spectrum has been fully assigned through IR-IR double resonance measurements employing a tunable, microwave sideband-CO2 laser. The 10 mu m spectrum of propargyl amine displays splittings in the two nuclear spin symmetry states arising from amino-proton interchange, allowing double-resonance assignment of the -NH2 group resultant proton nuclear spin quantum number in the highly fragmented 3 mu m spectrum. The experimental state density is consistent with a (2J + 1) increase that is expected if all near-resonant states are coupled. From this J-dependent growth in the state density we determine the density of states at J = 0 to be 22 states/cm(-1). This value is in reasonable agreement with the direct state count result of 16 states/cm(-1). The unperturbed transition frequencies for the two different nuclear spin species at a given rotational level do not coincide, differing on average by about 50 MHz. The nonresonant coupling effects which produce effective splittings in the 10 mu m spectrum appear to survive into the high state density regime. The measured IVR lifetimes are on the order of 500 ps for the low K-a values studied here (K-a < 4) and show a K-a-dependence with the IVR rate increasing as K-a increases. The statistical properties of the spectrum have been compared to predictions from random matrix theory. The level spacings are not well represented by Wigner statistics as would be expected for underlying chaotic classical dynamics. However, the intensity fluctuations are consistent with a chi(2)-distribution, expected for classically chaotic systems, as measured by Heller's F-statistic. (C) 1998 American Institute of Physics. [References: 49]
机译:炔丙基胺的炔属C-H拉伸光谱已在可调谐色心激光器中在共振光热光谱仪中以0.0002 cm(-1)(6 MHz)的分辨率测量到3330 cm(-1)附近。通过使用可调谐微波边带CO2激光器的IR-IR双共振测量,已完全分配了光谱。炔丙基胺的10μm光谱在两个核自旋对称状态下显示氨基-质子交换引起的分裂,从而允许在高度碎片化的3μm光谱中对-NH2基团生成的质子核自旋量子数进行双共振分配。如果耦合所有近共振状态,则实验状态密度与预期的(2J +1)增加一致。从状态密度中依赖于J的增长,我们确定J = 0时的状态密度为22个状态/ cm(-1)。此值与16个状态/ cm(-1)的直接状态计数结果在合理范围内。在给定的旋转水平下,两种不同核自旋物种的平稳扰动频率不一致,平均相差约50 MHz。在10微米光谱中产生有效分裂的非共振耦合效应似乎可以保留到高态密度体系中。对于此处研究的低K-a值(K-a <4),测得的IVR寿命约为500 ps,并显示出K-a依赖性,IVR速率随K-a的增加而增加。光谱的统计特性已与随机矩阵理论的预测进行了比较。 Wigner统计不能很好地表示水平间距,正如潜在的混沌经典动力学所期望的那样。但是,强度波动与经典混沌系统所期望的chi(2)分布一致,如通过Heller F统计量测得的。 (C)1998美国物理研究所。 [参考:49]

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