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The Rotational Spectroscopy of SrS Kerry C. Etchison, Chris T. Dewberry and Stephen A. Cooke Department of Chemistry, University of North Texas P.O. Box.

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Presentation on theme: "The Rotational Spectroscopy of SrS Kerry C. Etchison, Chris T. Dewberry and Stephen A. Cooke Department of Chemistry, University of North Texas P.O. Box."— Presentation transcript:

1 The Rotational Spectroscopy of SrS Kerry C. Etchison, Chris T. Dewberry and Stephen A. Cooke Department of Chemistry, University of North Texas P.O. Box 305070 Denton, TX 76203

2 Introduction Strontium is an alkaline earth metal, silvery white in appearance and has one isotope with nuclear spin. – 87 Sr 7.00% abundant I = 9/2 Strontium Sulfide has been the subject of two previous high resolution studies. –Rotational analysis of the A 1 Σ + -X 1 Σ + transition of SrS F. S. Pianalto, C. R. Brazier, L. C. O'Brien and P. F. Bernath. J. Mol. Spectrosc., 132, 80 (1988) –The pure rotational spectra of SrSH (X 2 A') and SrS (X 1 Σ + ): further studies in alkaline-earth bonding D.T. Halfen, A.J. Apponi, J.M. Thompsen, and L.M. Zuirys J. Chem. Phys., 115, 11131 (2001)

3 Experimental Method

4

5 Our Spectrometer

6 Our Spectrometer Circuit

7 The Walker-Gerry Ablation Nozzle

8 The Strontium Rod OCS was used as the precursor gas.

9 Our Results

10 Example of what we see: 88 Sr 32 S 350 Avg. Cycles J = 2-1 v = 1 after 548 shots

11 Summary of data collected Spectra of four isotopomers – 88 Sr 32 S J = 1-0 v = 0, 1, and 2 J = 2-1 v = 0, 1, 2, and 3 J = 3-2 v = 0 and 1 – 87 Sr 32 S J = 2-1 v = 0 J = 3-2 v = 0 – 86 Sr 32 S J = 2-1 v = 0 and 1 J = 3-2 v = 0 – 88 Sr 34 S J 3-2 v = 0

12 Table of Data Collected

13 Spectral Analysis For the 87 Sr 32 S isotopomer we used SPFIT for the initial analysis of the data. This was followed by prediction of hypothetical line centers for each v, (J+1) - J transition observed. These line centers together with the rest of the data set and also the data of Halfen, et al. were then used in a Dunham- type analysis.

14 Three areas to discuss: 1. The quadrupole coupling constants 2. The Dunham analysis 3. The Born-Oppenheimer Breakdown terms in SrS

15 Quadrupole Coupling Constants eQq ( 87 Sr) 87 Sr 16 O/MHz-42.729(37) 87 Sr 32 S/MHz-21.959(85)

16 The Dunham Analysis In our analysis we have followed Watson’s formalism in which:

17 The Dunham Analysis r e BO (SrS) = 2.4397188(21) Å

18 Born-Oppenheimer Breakdown Terms AB ∆∆ U01 / u MHz HCl-0.26(20)0.1262(8)311077.90(96) CO-2.0545(12)-2.0982397029.003(24) ZrS-5.325(82)-6.523(39)108670.07(19) GeS-1.463(70)-1.871(45)124836.77(12) SrS-0.78(30)-3.77(57)84906.76(15) A 01 B 01

19 Conclusions The pure rotational spectra of four isotopomers of SrS have been measured in their electronic ground states on a newly constructed laser ablation, FTMW spectrometer. The quadrupole coupling constant for Sr in SrS has been determined for the first time. A multi-isotopomer analysis has allowed the determination of the Born-Oppenheimer breakdown terms for Sr and S in SrS.

20 Acknowledgements ACSWC 2007 Travel Grant PRF Type G Ralph E. Powe Junior Faculty Enhancement Award UNT Mech. Workshop

21 The Cooke Group

22 The UNT New Chemistry Building


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