THE $b{^{3}}\Pi_{u0}$ STATE OF $^{39}K_{2}$

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2002

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Ohio State University

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New observations of the b3Πu0 state of K2 have been made by laser induced fluorescence spectroscopy, following single colour OODR excitation with a cw Ti:sapphire laser. Fourier transform spectra revealed two pieces of a progression of the 23Πgb3Πu0 system, beginning around 14250 cm−1, at v=0, and terminating at 7200 cm−1. The two pieces were unfortunately separated by very strong AX emission, which dominated the region 8000−12000cm−1, so that no measurements could be made for many intermediate vibrational levels. The triplet emission in the visible region was severely affected by spin-orbit interactions with A1Σu+, whilst the infrared part of the spectrum was much less perturbed. The intermediate part of the potential is known only through the interactions of the A1Σu+ and b3Πu states. The spin-orbit interaction between the A and b states up to vb=90 has been modelled using an ab initio calculation of the spin-orbit function, which shows a notable dip as a function of R. This model allowed us to assign the vibrational quantum numbers in the infrared part of the fluorescence spectrum : the observations cover 89≤v≤118. We are fitting the available A and b state data to Yij parameters. At present, we have achieved fits (with a standard deviation of 0.025cm−1) of about 1000 term values or combination differences, corresponding to levels up to 5500cm−1 above the minimum of the b state. We intend to continue the fits over a further 1500cm−1 to incorporate all the data, reaching term values 500cm−1 below the 4S + 4P threshold. An asymptotic calculation of the Hund's case c) 0u+ states should be able to extend a deperturbed potential curve for the b state sufficiently accurately to allow the assignment of existing photoassociation data.

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Author Institution: Laboratoire de Spectrom'{e}trie Ionique et Mol'{e}culaire (UMR 5579 CNRS), B^{a}timent Kastler, Universit'{e} Lyon I, Domaine Scientifique de la Doua; Department of Physics, Temple University; Department of Modern Applied Physics, Tsinghua University; Department of Physics and Astronomy, State University of New York; Laboratoire Aim'{e} Cotton (CNRS UPR3321), Campus d'Orsay; Energetic Materials Center.Lawrence Livermore National Laboratory, University of California

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