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Molecular Dynamics in Hydrogen‐bonded Interactions: A Preliminary Experimentally Determined Harmonic Stretching Force Field for HCN‐‐‐HF

机译:氢键相互作用的分子动力学:HCN --- HF的初步实验确定的谐波拉伸力场

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摘要

Observation of the 2ν1 overtone band in the hydrogen‐bonded complex HCN‐‐‐HF permits evaluation of the anharmonicity constant X 1 1=−116.9(1) cm− 1 and determination of the anharmonicity corrected fundamental frequency ω1. This information, and available data from previous rovibrational analyses in the common and perdeuterated isotopic species of HCN‐‐‐HF, offer an opportunity for calculation of an approximate stretching harmonic force field. With the assumptions f 1 2=f 2 4=0.0, the remaining force constants (in mdyn/Å) are evaluated as: f 1 1=8.600(20), f 2 2=6.228(9), f 3 3=19.115(40), f 4 4=0.2413(39), f 1 3=0.000(13), f 1 4=0.0343(2), f 2 3=−0.211(6), f 3 4=0.000(2). These compare to f 1 1=9.658(2) in the HF monomer and f 1 1=6.244(3) and f 3 3=18.707(16) in the HCN monomer. These results provide the information necessary to quantitatively assess the applicability of the Cummings and Wood approximation in this hydrogen‐bonded complex and also give an estimate of D e j , the equilibrium distortion constant in the harmonic limit. Comparisons of these experimentally determined parameters with the predictions of a b i n i t i o molecular orbital calculations at several levels of approximation are presented.
机译:观察氢键复合HCN-HF中的2ν1泛音带,可以评估非谐波常数X 1 1 = -116.9(1)cm-1,并确定经非谐波校正的基频ω1。该信息以及以前在HCN-HF的常见和氘代同位素中进行的振动分析得出的数据,为计算近似拉伸谐波力场提供了机会。假设f 1 2 = f 2 4 = 0.0,剩余力常数(以mdyn /Å表示)为:f 1 1 = 8.600(20),f 2 2 = 6.228(9),f 3 3 = 19.115 (40),f 4 4 = 0.2413(39),f 1 3 = 0.000(13),f 1 4 = 0.0343(2),f 2 3 = -0.211(6),f 3 4 = 0.000(2)。这些与HF单体中的f 1 1 = 9.658(2)和HCN单体中的f 1 1 = 6.244(3)和f 3 3 = 18.707(16)相比。这些结果为定量评估卡明斯和伍德近似在这种氢键配合物中的适用性提供了必要的信息,并提供了D e j的估计值,即谐波极限中的平衡畸变常数。这些实验确定的参数与几种近似水平下的分子轨道计算的预测值进行了比较。

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