Elsevier

Chemical Physics Letters

Volume 318, Issues 4–5, 25 February 2000, Pages 454-458
Chemical Physics Letters

The first spectroscopic observation of YbS: the A0+–X0+ visible laser excitation spectrum

https://doi.org/10.1016/S0009-2614(00)00035-XGet rights and content

Abstract

The first spectroscopic observation of YbS has been made using visible laser excitation spectroscopy. Gas-phase YbS was produced in a Broida oven by the reaction of Yb metal vapour with either CS2 or OCS. Dispersed fluorescence spectra of an Ω=0–Ω=0 electronic transition were recorded with a CCD array detector. A least-squares fit of 34 band-heads leads to the following molecular parameters for the lower state: ωe″=365.6(2) cm−1 and ωexe″=1.14(2) cm−1. Determination of the parameters for the upper state of the transition was precluded by the irregular vibrational spacings, which increased with increasing v′.

Introduction

The visible absorption spectra of numerous lanthanide-containing diatomic molecules have been studied over the last twenty years. In particular, a great deal of progress has been made in probing the electronic structure of rare-earth monoxides, both experimentally 1, 2, 3, 4, 5, 6, 7, 8and theoretically 9, 10, 11, 12, 13, 14. Part of the motivation for this work lies in the fact that molecules containing a lanthanide atom offer a unique opportunity to examine both open and closed f-shell electronic configurations.

The ground state of the ytterbium atom has the closed-shell electron configuration (Xe) 4f146s2, and is therefore similar to an alkaline-earth atom, but with the addition of a filled 4f-subshell. Experimental 8, 15, 16and theoretical 11, 12, 13, 17, 18, 19work on YbO have revealed the presence of two low-lying electronic configurations, Yb2+(4f14)O2− and Yb2+(4f136s)O2−. Experimentally, the ground state of YbO has been found to have 0+ symmetry (in Hund's case (c) notation), and is attributed to the 4f14 configuration [15].

Although there has been no report of a spectroscopic study of YbS, a recent density functional (DF) investigation concluded that the ground state of YbS arises from the 4f14 configuration [19], the same as that found in YbO. The present work was undertaken to extend the fragmentary information available on rare-earth containing compounds and to test the validity of the conclusions in the DF study of Liu et al. [19].

While sulfur exists naturally in 4 isotopes, 32S (95.0%), 33S (0.75%), 34S (4.2%) and 36S (0.02%), ytterbium is present in nature as a mixture of 7 isotopes, 6 of which have >1% abundance. The spectroscopic resolution of the current work is not sufficient to resolve transitions of different Yb isotopomers of YbS, though several bands of the minor isotopomers Yb33S and Yb34S were observed.

Section snippets

Experimental method

Gas-phase YbS molecules were produced in a Broida-type [20]oven by the reaction of Yb metal vapour in a flow of argon carrier gas with either CS2 or OCS. Though both oxidant gases produced a sufficient amount of YbS to study using laser spectroscopy, the most stable conditions, and best S/N, were for OCS. Total pressures in the oven were kept at 3–5 Torr, and typically ∼10 mTorr of oxidant was required. The products were probed using the output of a Coherent 599 dye laser operating in broadband

Results and discussion

The YbS laser excitation spectra obtained in the present work consist of a large number of red-degraded bands in the range 560–600 nm. Fig. 1 shows a portion of the spectrum containing the Δv=1 sequence. Most of the 34 bands recorded were assigned to the principal isotopomer, Yb32S, while a few heads of the minor isotopomers Yb33S and Yb34S were recorded for the 0–1 and 0–2 bands, confirming the carrier of the present spectra as YbS. Band-heads and the corresponding isotope shifts for the minor

Acknowledgements

We thank Professor Colan Linton (University of New Brunswick) for several helpful discussions. T.C.M. thanks Dalhousie University and the Walter C. Sumner Foundation for graduate scholarships. Support for this work via a Research Grant from the Natural Sciences and Engineering Research Council of Canada is gratefully acknowledged.

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