首页> 外文期刊>Journal of Molecular Structure. Theochem: Applications of Theoretical Chemistry to Organic, Inorganic and Biological Problems >Rotationally inelastic collisions of LiH (X~1Σ~+) with H: State-to-state inelastic rotational cross-section
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Rotationally inelastic collisions of LiH (X~1Σ~+) with H: State-to-state inelastic rotational cross-section

机译:LiH(X〜1Σ〜+)与H的旋转非弹性碰撞:状态间的非弹性旋转横截面

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The potential energy surface describing the interaction between the hydrogen atom and the rotating LiH molecule has been calculated very accurately and presented in our previous work (J. Mol. Struct. (THEOCHEM) 678 (2004) 11). The rigid rotor potential already fitted analytically and expanded in terms of Legendre polynomials, is employed here to evaluate the pure state-to-state rotational cross-sections over a range of energies of astrophysical interest varying from 10 to 3000 cm?1. An exact close coupling and CS calculation of the state to state rotational cross-section was done first in the range of small energy, from 10 to 100 cm?1. The comparison of both results shows the good agreement between them and leads to a generalisation of such calculation for higher energy using the CS approximation. We determine the state to state rotational cross-section for transitions from j=0, 1, 2, 3, 4 to all accessible final states j′, at total energy varying between 10 and 3000 cm~(-1). The presented cross-sections were found to be very large even for low energy and large Δ_(jj′). Thus indicates the important probability to produce the heated LiH molecule in excited states by collisions with H and explain the strong anisotropy discussed in our previous paper.
机译:描述氢原子和旋转的LiH分子之间相互作用的势能面已经非常精确地计算出来,并在我们以前的工作中提出(J. Mol。Struct。(THEOCHEM)678(2004)11)。刚性转子电势已经通过解析拟合并根据勒让德多项式进行了扩展,在这里用于评估天体感兴趣的能量范围从10到3000 cm?1的纯状态到状态的旋转截面。首先在10至100 cm?1的小能量范围内进行精确的紧密耦合和状态到状态旋转截面的CS计算。两种结果的比较显示了它们之间的良好一致性,并导致使用CS近似对较高能量进行这种计算的一般化。我们确定了从j = 0、1、2、3、4到所有可到达的最终状态j'的过渡状态到状态的旋转截面,总能量在10和3000 cm〜(-1)之间变化。发现所呈现的横截面即使对于低能量和大Δ_(jj')也非常大。因此表明了通过与H的碰撞产生处于激发态的加热的LiH分子的重要可能性,并解释了我们先前论文中讨论的强各向异性。

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