Dissociation dynamics of the methylsulfonyl radical and its photolytic precursor CH3SO2Cl
J. Chem. Phys. 131, 044305 (2009); doi:10.1063/1.3159555
Published 22 July 2009
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The dissociation dynamics of methylsulfonyl radicals generated from the photodissociation of CH3SO2Cl at 193 nm is investigated by measuring product velocities in a crossed laser-molecular beam scattering apparatus. The data evidence three primary photodissociation channels of the precursor: S–Cl fission to produce Cl atoms and ground electronic state CH3SO2 radicals, S–Cl fission to produce Cl atoms and electronically excited CH3SO2 radicals, and S–CH3 fission. Some of the vibrationally excited CH3SO2 radicals undergo subsequent dissociation to CH3+SO2, as do all of the electronically excited radicals. The velocities of the SO2 products show that the vibrationally excited ground state CH3SO2 radicals dissociate via a loose transition state having a small exit barrier beyond the endoergicity. Hence, a statistical recoil kinetic energy distribution should and does fit the distribution of velocities imparted to these SO2 products. The electronically excited CH3SO2 radicals also dissociate to CH3+SO2, but with a larger average release to relative kinetic energy. Interestingly, when using 200 eV electron bombardment detection, the ground electronic state CH3SO2 radicals having too little internal energy to dissociate are not observed at the parent CH3SO
ion, but only at the CH
daughter ion. They are distinguished by virtue of the velocity imparted in the original photolytic step; the detected velocities of the stable radicals are consistent with the calculated barrier of 14.6 kcal/mol for the dissociation of CH3SO2 to CH3+SO2. We present CCSD(T) calculations of the adiabatic excitation energy to the lowest excited state of CH3SO2 radicals, the 1 2A
state, as well as the vertical energy from the equilibrium geometry of that excited state to the 2 2A
state, to aid in the experimental assignment.
©2009 American Institute of Physics
state, as well as the vertical energy from the equilibrium geometry of that excited state to the 2 2A
state, to aid in the experimental assignment.
©2009 American Institute of Physics
| History: | Received 11 November 2008; accepted 19 March 2009; published 22 July 2009 |
| Permalink: |
http://link.aip.org/link/?JCPSA6/131/044305/1 |
EDITORIALLY RELATED
- Determining the CH3SO2
CH3+SO2 barrier from methylsulfonyl chloride photodissociation at 193 nm using velocity map imaging
Britni J. Ratliff et al.
J. Chem. Phys. 131, 044304 (2009)
EPAPS
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KEYWORDS and PACS
RELATED DATABASES
PUBLICATION DATA
0021-9606 (print)
1089-7690 (online)
REFERENCES (23)
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- M. Speidel, R. Nau, F. Arnold, H. Schlager, and A. Stohl,
Atmos. Environ. 41, 2427 (2007) . - A. Saltelli and J. Hjorth,
J. Atmos. Chem. 21, 187 (1995) . - S. B. Barone, A. A. Turnipseed, and A. R. Ravishankara,
Faraday Discuss. 100, 39 (1995) . - A. J. Frank and F. Turecek,
J. Phys. Chem. A 103, 5348 (1999) . - L. Zhu and J. W. Bozzelli,
J. Mol. Struct.: THEOCHEM 728, 147 (2005) . - J. C. Owrutsky, H. H. Nelson, and A. P. Baronavski,
J. Phys. Chem. A 105, 1440 (2001) . - B. J. Ratliff, X. N. Tang, L. J. Butler, D. E. Szpunar, and K. -C. Lau, 131, 044304 (2009).
- J. M. L. Martin, J. Chem. Phys. 108, 2791 (1998).
- D. Borissenko, A. Kukui, G. Laverdet, and G. Le Bras,
J. Phys. Chem. A 107, 1155 (2003) . - A. Ray, I. Vassalli, G. Laverdet, and G. Le Bras,
J. Phys. Chem. 100, 8895 (1996) , and earlier references within. - A. Kukui, V. Bossoutrot, G. Laverdet, and G. Le Bras,
J. Phys. Chem. A 104, 935 (2000) . - Y. T. Lee, J. D. McDonald, P. R. LeBreton, and D. R. Herschbach, Rev. Sci. Instrum. 40, 1402 (1969).
- N. R. Daly, Rev. Sci. Instrum. 31, 264 (1960).
- See EPAPS supplementary material at http://dx.doi.org/10.1063/1.3159555 for energies, geometries, and moments of inertia of the intermediates and transition states for the CH3SO2 potential energy surface, calculated at the G3//B3LYP level of theory, along with supplemental experimental data. The second supplementary file gives the optimized geometry of the lowest doublet excited state of CH3SO2 calculated at the CCSD(T) level of theory described herein. [EPAPS]
- A. G. Baboul, L. A. Curtiss, P. C. Redfern, and K. Raghavachari, J. Chem. Phys. 110, 7650 (1999).
- M. J. Frisch, G. W. Trucks, H. B. Schlegel et al., GAUSSIAN03, Revision C.02 Gaussian, Inc., Pittsburgh, PA, 2003.
- J. F. Stanton, J. Gauss, J. D. Watts, P. G. Szalay, and R. J. Bartlett, with contributions from A. A. Auer, D. E. Bernholdt, O. Christiansen, M. E. Harding, M. Heckert, O. Heun, C. Huber, D. Jonsson, J. Jusélius, W. J. Lauderdale, T. Metzroth, C. Michauk, D. P. O'Neill, D. R. Price, K. Ruud, F. Schiffmann, M. E. Varner, J. Vázquez and the integral packagesby J. Almlöf and P. R. Taylor, MOLECULE, P. R. Taylor, PROPS, and T. Helgaker, H. J. Aa. Jensen, P. Jørgensen, and J. Olsen, ABACUS. For the current version, see http://www.aces2.de.
- H. -J. Werner, P. J. Knowles, R. Lindh et al., MOLPRO, version 2006.1, a package of ab initio programs, see http://www.molpro.net.
- R. E. Center and A. Mandl, J. Chem. Phys. 57, 4104 (1972).
- T. M. Miller and B. Bederson,
Adv. At. Mol. Phys. 13, 1 (1977) . - J. J. Lin, private communication, 2001. Daughter fragmentation pattern of methyl radicals upon 70 eV electron bombardment detection from the photodissociation of CH3I at 157 nm, dispersing the methyl radicals as a function of internal energy from 3 to 88 kcal/mol in 5 kcal/mol increments.
- C. Chatgilialoglu, D. Griller, and M. Guerra,
J. Phys. Chem. 91, 3747 (1987) . - L. A. Curtiss, P. C. Redfern, K. Raghavachari, and J. A. Pople, J. Chem. Phys. 114, 108 (2001).








