12–17 Jun 2016
University of Ottawa
America/Toronto timezone
Welcome to the 2016 CAP Congress! / Bienvenue au congrès de l'ACP 2016!

FTIR Synchrotron Spectroscopy of the Lower Vibrational Modes of Methyl Mercaptan at the Canadian Light Source

13 Jun 2016, 16:45
15m
Colonel By D207 (University of Ottawa)

Colonel By D207

University of Ottawa

Oral (Non-Student) / orale (non-étudiant) Division of Atomic, Molecular and Optical Physics, Canada / Division de la physique atomique, moléculaire et photonique, Canada (DAMOPC-DPAMPC) M3-2 Atomic and Molecular Spectroscopy and Precision Measurements II (DAMOPC) / Spectroscopie atomique et moléculaire et mesures de précision II (DPAMPC)

Speaker

Dr Ronald M. Lees (Physics Dept., University of New Brunswick)

Description

The Fourier transform infrared spectra of the lower infrared vibrational bands of CH$_{3}$SH have been investigated from 650 to 1200 cm$^{-1}$ at 0.001 cm$^{-1}$ resolution employing synchrotron radiation at the Canadian Light Source in Saskatoon. The relative band strengths and structures are remarkably different from those for the analogous CH$_{3}$OH relative, with the CSH bend being very weak and both the in-plane and out-of-plane CH$_{3}$ rocks being strong with comparable intensities. The CSH bend has parallel $a$-type character with no detectable $b$-type component. The out-of-plane CH$_{3}$ rock is a purely $c$-type perpendicular band, whereas the in-plane rock around is of $a$/$b$ character. The $K$-reduced $v_{t}$ = 0 sub-state origins for the CSH bend follow the normal oscillatory torsional pattern as a function of $K$ with an amplitude of 0.362 cm$^{-1}$, as compared to 0.653 cm$^{-1}$ for the ground state and 0.801 cm$^{-1}$ for the C-S stretching mode. The torsional energy curves for the out-of-plane rock are also well-behaved but are inverted, with an amplitude of 1.33 cm$^{-1}$. In contrast, the sub-state origins for the in-plane rock do not display a clear oscillatory structure but are scattered over a range of about 2 cm$^{-1}$, with indications of some significant perturbations. Our sub-band assignments extend up to about $K$ = 10 for all the modes and are well-determined from GSCD relations, particularly for the $a$/$b$ in-plane rock for which $\Delta$$K$ = 0, +1 and $-$1 transitions are all observed.

Author

Dr Ronald M. Lees (Physics Dept., University of New Brunswick)

Co-authors

Dr Brant E. Billinghurst (Canadian Light Source) Dr Li-Hong Xu (Physics Dept., University of NB)

Presentation materials