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HIGH-RESOLUTION INFRARED SPECTROSCOPY OF ISOTOPIC IMPURITY Q(1)(0) TRANSITIONS IN SOLID PARAHYDROGEN

机译:固体副烃中同位素杂质Q(1)(0)跃迁的高分辨率红外光谱

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We have made a high-resolution infrared spectroscopic study of the Q(1)(0) (v = 1 <-- 0, J = 0 <-- 0) vibrational transitions of the isotopic impurities D-2 and HD in solid parahydrogen. Each impurity has a spectrum composed of similar to 100 sharp lines spread over similar to 0.4 cm(-1). The linewidths vary, but are on the order of 10 MHz. These spectra make clear: (1) the infrared Q(1)(0) transitions of J = 0 isotopic impurities are induced by the quadrupolar fields of nearby impurity J = 1 molecules; and (2) the spectral pattern of strong Q(1)(0) lines is due to the splitting of the M-orientational levels of J = 1/J = 0 o-D-2 or J = 1/J = 0 HD nearest-neighbor (nn) impurity pairs. With the aid of several theoretical works, the strong lines in the D-2 and HD spectra can be individually and unambiguously assigned as specific quantum state Q(1)(0) transitions of nn impurity pairs containing p-D-2/o-D-2 or o-H-2/o-D-2, and o-H-2/HD, respectively. The assigned transitions of nn impurity pairs containing the o-H-2 are confirmed by combination differences which agree to within 5 x 10(-4) cm(-1), the instrumental precision. These assignments yield complete Q(1)(0) energy level diagrams for the nn impurity pairs o-H-2/o-D-(2) and o-H-2/HD embedded in solid parahydrogen. The experimental energy level splittings are fit to a two parameter model which describes anisotropic interactions in the parahydrogen crystal. These experimental parameters appear to have significant contributions from the changes in renormalization and lattice constant around the heavier isotopic impurity. We have also assigned a few of the weaker spectral features as Q(1)(0) transitions of more distant impurity pairs, but the bulk of these transitions are yet to be assigned, They do form a distinctive pattern and are thought to be the Q(1)(0) transitions of impurity triples and larger clusters, This study is one of the few cases for which high-resolution laser spectroscopy has been successfully applied to the condensed phase and for which many of the transitions have rigorous quantum state assignments. (C) 1996 American Institute of Physics. [References: 72]
机译:我们对固体对氢中同位素杂质D-2和HD的Q(1)(0)(v = 1 <-0,J = 0 <-0)振动跃迁进行了高分辨率红外光谱研究。每种杂质的光谱均由分布在0.4 cm(-1)左右的100条清晰的线条组成。线宽有所不同,但约为10 MHz。这些光谱清楚地表明:(1)J = 0同位素杂质的红外Q(1)(0)跃迁是由附近杂质J = 1分子的四极场引起的; (2)强Q(1)(0)线的频谱图是由于M原始水平的分裂,即J = 1 / J = 0 oD-2或J = 1 / J = 0 HD最接近-邻居(nn)个杂质对。借助一些理论工作,可以将D-2和HD光谱中的强线分别明确地指定为nn个包含pD-2 / oD-2或Pd-2 / oD-2的杂质对的特定量子态Q(1)(0)跃迁。 oH-2 / oD-2和oH-2 / HD。包含o-H-2的nn个杂质对的分配跃迁通过组合差异确认,该差异在仪器精度5 x 10(-4)cm(-1)内。这些分配为嵌入固体对氢中的nn个杂质对o-H-2 / o-D-(2)和o-H-2 / HD提供了完整的Q(1)(0)能级图。实验的能级分裂适合两个参数模型,该模型描述了对氢晶体中的各向异性相互作用。这些实验参数似乎是由于重同位素杂质周围的重归一化和晶格常数变化而产生的重要贡献。我们还分配了一些较弱的光谱特征作为距离较远的杂质对的Q(1)(0)跃迁,但是这些跃迁的大部分尚未分配,它们确实形成了独特的模式,被认为是杂质三元组和较大簇的Q(1)(0)跃迁,本研究是将高分辨率激光光谱成功应用于凝聚相且其中许多跃迁具有严格的量子态分配的少数情况之一。 (C)1996年美国物理研究所。 [参考:72]

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