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首页> 外文期刊>Optics and Spectroscopy >Semiempirical Study of Perturbations of the Lande g Factors of ElectronicVibrationalRotational Levels of Hydrogen: II. i~3Π_g~- and j~3Δ_g~- States of the H_2, HD, and D_2 Molecules
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Semiempirical Study of Perturbations of the Lande g Factors of ElectronicVibrationalRotational Levels of Hydrogen: II. i~3Π_g~- and j~3Δ_g~- States of the H_2, HD, and D_2 Molecules

机译:氢电子振动旋转能级的Lande g因子摄动的半经验研究:II。 H_2,HD和D_2分子的i〜3Π_g〜-和j〜3Δ_g〜-状态

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The values of the Lande g factors of the i~3Π_g~- v, N and j~3Δ_g~-, v, N states of the H_2, HD, and D_2 molecules have been found semiempirically for the following vibrational and rotational quantum numbers: v ≤ 3; N ≤ 7 for H_2; N ≤ 5 for HD; and N ≤ 11 for D_2. These values were obtained in terms of the nonadiabatic model, which takes into account the interaction between the 3dπ~3Πg and 3d3δ~Δg states with the same values of and N in the approximation of pure precession, with the use of semiempirical values of the expansion coefficients of the wave functions in the Born–Oppenheimer basis determined by us previously and the results of numerical calculation of the overlap integrals of the vibrational wave functions of these states. The results obtained for the H_2 molecule are in good agreement with the data in the literature. For the i~3Π_g~- and j~3Δ_g~- states of the HD and D_2 molecules, the g factors were found for the first time. This made it possible to study for the first time the role of the isotopic effect in the perturbation of the dependences of the g factors of rovibrational levels on and N for the triplet electronic states of the hydrogen molecule. It was found that the interference effects of interaction between the 3d3g and 3d3g states lead both to significant differences-up to 8, 6, and 11 times for H_2, HD, and D_2, respectively (the i~3Π_g~- state), 20 times for H_2 and HD, and two orders of magnitude for D_2 (the i~3Δ_g~- state)—between the nonadiabatic values of the g factors and the corresponding adiabatic values for some isotopomers of the hydrogen molecule and to significant differences-up to 9 and 1.5 times for the i~3Δ_g~- and i~3Π_g~- states, respectively-in the nonadiabatic values of the g factors of rovibrational levels of different isotopomers of the hydrogen molecule.
机译:对于以下振动和旋转量子数,半经验地找到了H_2,HD和D_2分子的i〜3Π_g〜-v,N和j〜3Δ_g〜-,v,N状态的Lande g因子值: v≤3;对于H_2,N≤7;对于高清,N≤5;对于D_2,N≤11。这些值是根据非绝热模型获得的,该模型考虑了3dπ〜3Πg和3d3δ〜Δg状态之间的相互作用,其中n和N的值相同,在纯粹进动的近似中,使用展开的半经验值我们先前确定的在Born–Oppenheimer基础上的波动函数的系数,以及这些状态的振动波动函数的重叠积分的数值计算结果。 H_2分子获得的结果与文献中的数据非常吻合。对于HD和D_2分子的i〜3Π_g〜-和j〜3Δ_g〜-状态,首次发现了g因子。这使得首次研究同位素效应在扰动振动能级的g因子对氢分子的三重态电子态和N的依赖关系中的作用成为可能。发现3d3g和3d3g状态之间相互作用的干扰效应导致H_2,HD和D_2(i〜3Π_g〜-状态)的差异分别高达8、6和11倍,分别为20 H_2和HD的时间,以及D_2(i〜3Δ_g〜-状态)的两个数量级-在g因子的非绝热值与氢分子的某些同分异构体的相应绝热值之间,并且直至在氢分子的不同同分异构体的振动水平的g因子的非绝热值中,i〜3Δ_g〜-和i〜3Π_g〜-状态分别是9和1.5倍。

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