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Structure and energy difference of two isomers of He-CH_3F

机译:He-CH_3F的两种异构体的结构和能差

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The intermolecular potential surface of He-CH_3F is investigated through ab initio calculations and microwave and millimeter-wave spectroscopies.The intermolecular potential is calculated at the fourth-order M011er-Plesset level with a large basis set including bond functions.Three minimums exist,the deepest of which is at the carbon end of the C-F axis and has a depth of 46.903 cm~(-1),the second deepest is in a T-shaped position relative to the C-F axis with a depth of 44.790 cm~(-1),and the shallowest is at the fluorine end of the C-F axis with a depth of 30.929 cm~(-1).The barrier to internal rotation of the CH_3F subunit about its C-F axis is very low,thus leading to essentially free internal rotation and two separate sets of bound states correlating to ortho-CH_3F (|K|=3n) for the ground,or A,internal rotor state upon which this study focuses,and to para-CH_3F (|K|=3n+-1) for the excited,or E,internal rotor state.Bound-state calculations of the A state performed using two different techniques show the lowest-energy state to have the helium localized in the T-shaped well with an energy of -11.460 cm~(-1),while two excited configurations of the A state have the helium localized either in the well at the carbon end ("linear") with an energy of -7.468 cm~(-1) or in the well at the fluorine end ("antilinear") with an energy of -4.805 cm~(-1).Spectroscopic observations confirm the predicted energy-level structure of the ground and first excited states.Sixteen transitions between 12 distinct energy levels have been observed,including pure rotational transitions of both the T-shaped ground state and the linear excited state,as well as rovibrational transitions between the ground state and the linear excited state.The energy difference between the T-shaped state and the linear state is measured to be 132 374.081(16) MHz.There is significant Coriolis mixing of the ground state J_(K_aK_c)=2_(20) and the linear J_K=2_0 levels which aided in the observation of the T to linear transitions.This mixing and the T to linear energy difference are sensitive probes of the relative well depths of the two lowest minimums and are well predicted by the ab initio potential.Improved agreement between experiment and theory is obtained by morphing the correlation energy of the potential.He-CH_3F is one of just a few atom-molecule complexes for which the ground-state geometry does not coincide with the global potential minimum.
机译:通过从头算以及微波和毫米波光谱学方法研究了He-CH_3F的分子间电势表面。分子间电势是在四阶M011er-Plesset能级下计算的,其中大的基础包括键函数。存在三个最小值其中最深的是CF轴的碳端,深度为46.903 cm〜(-1),第二最深的是相对于CF轴处于T形位置,深度为44.790 cm〜(-1) ),最浅的是CF轴的氟末端,深度为30.929 cm〜(-1).CH_3F亚基绕其CF轴的内部旋转的障碍非常低,因此导致内部自由旋转以及两组独立的结合状态,它们分别与本研究关注的地面或A,内部转子状态和邻CH_3F(| K | = 3n)相关,并与对位CH_3F(| K | = 3n + -1)相关励磁或E转子内部状态。使用两种不同的方法对A状态进行边界状态计算nt技术显示能量最低的状态是将氦定位在T型井中,能量为-11.460 cm〜(-1),而两种激发态的A状态的氦都定位在T型井中。碳末端(“线性”)的能量为-7.468 cm〜(-1),或者在井中的碳末端(“线性”)的能量为-4.805 cm〜(-1)。光谱观察证实了预测的结果。基态和第一激发态的能级结构。已观察到12种不同能级之间的十六个跃迁,包括T形基态和线性激发态的纯旋转跃迁以及基态之间的振动跃迁T形态和线性态之间的能量差经测量为132 374.081(16)MHz。基态J_(K_aK_c)= 2_(20)和线性J_K = 2_0电平有助于观察T到lin这种混合和T到线性能量差是两个最低最小值的相对阱深度的灵敏探针,并且可以通过从头算势来很好地预测。通过使电子束的相关能变形,可以提高实验与理论之间的一致性。 He-CH_3F是仅有的几种原子-分子配合物之一,其基态几何形状与全局最小电位不符。

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