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首页> 外文期刊>The Journal of Chemical Physics >The ground X 1∑_g~+electronic state of the cesium dimer: Application of a direct potential fitting procedure
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The ground X 1∑_g~+electronic state of the cesium dimer: Application of a direct potential fitting procedure

机译:铯二聚体的接地X1∑_g~+电子态:应用直接电位拟合程序

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摘要

A collection of 16 544 fluorescence series spectroscopic line positions involving the A 1∑_u~+→X 1∑_g~+ transition in Cs_2 has been analyzed by a modern direct potential fitting procedure togenerate the first fully analytical potential energy function for the ground electronic state, and precise energy term values for the excited A ~1∑_u~+ state. The potential function yields an accuraterepresentation of spectroscopic data that span 99.24 of the well depth and the number of fitted parameters is significantly less than half the number of parameters determined in conventional Dunham analyses. A novel variant of the Morse/long-range potential model has been employed in the representation of the ground state potential, and a critical comparison has been made with an extended modified Lennard-Jones potential model. Proper account has been taken of the knownlong-range van der Waals form of the potential, and our final potential function is determined with constrained literature values of the C_8 and C_10 dispersion energy coefficients, along with a fittedvalue of C_6=3.31(5)×107 cm~(-1) A~6=6870(100) a.u. The fitted dissociation energy (D_e)is compared with the precisely known value based on the recent analysis of data from a two-photontransfer process (STIRAP)in ultracold Cs atoms. It is concluded that hyperfine effects in the X 1∑_g~+state are not negligible, and that the estimate of D_e=3649.84(7) cm~(-1) obtained in this workrepresents an effective dissociation limit lying between the two lowest hyperfine limits. Precise rotational and centrifugal distortion constants for the ground electronic state have also beencalculated through conventional perturbation theory. These estimates are fully consistent with the derived potential function and the experimental spectroscopic information.

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