Photodissociation of acryloyl chloride at 193 nm: interpretation of the product energy distributions, and new elimination pathways

2016 ◽  
Vol 18 (6) ◽  
pp. 5019-5026 ◽  
Author(s):  
Raúl Pérez-Soto ◽  
Saulo A. Vázquez ◽  
Emilio Martínez-Núñez

The use of an automated TS search method leads to the finding of novel HCl elimination pathways.

2004 ◽  
Vol 120 (9) ◽  
pp. 4223-4230 ◽  
Author(s):  
D. E. Szpunar ◽  
J. L. Miller ◽  
L. J. Butler ◽  
F. Qi

2002 ◽  
Vol 106 (34) ◽  
pp. 7728-7735 ◽  
Author(s):  
Katsuyoshi Yamasaki ◽  
Akihiro Watanabe ◽  
Teruaki Kakuda ◽  
Akira Itakura ◽  
Hirofumi Fukushima ◽  
...  

1994 ◽  
Vol 98 (1) ◽  
pp. 122-125 ◽  
Author(s):  
Haruki Ishikawa ◽  
Okitsugu Kajimoto
Keyword(s):  

2020 ◽  
Author(s):  
Bethan Nichols ◽  
Erin Sullivan ◽  
Daniel Neumark

<p>The photodissociation dynamics of the <i>tert</i>-butyl perthiyl (<i>t</i>-BuSS) radical are investigated by fast-beam coincidence translational spectroscopy. A fast (6-8 keV) beam of neutral <i>t</i>-BuSS radicals is produced via photodetachment of the corresponding anion, followed by photodissociation at 248 nm (5.00 eV) or 193 nm (6.42 eV) and coincident detection of the neutral products. Photofragment mass and translational energy distributions are obtained at both wavelengths. At 248 nm, the dominant product channel (90%) is found to be S loss, with a product translational energy distribution that peaks close to the maximum available energy and an anisotropic photofragment angular distribution, indicating dissociation along a repulsive excited state. A minor channel (10%) leading to the formation of S<sub>2</sub> + <i>t</i>-Bu is also observed. At 193 nm, both two- and three-body dissociation are observed. Formation of S<sub>2</sub> + <i>t</i>-Bu is the dominant two-body product channel, with multiple electronic states of the S<sub>2</sub> molecule produced via excited state dissociation processes. Formation of S + <i>t</i>-BuS is a minor two-body channel at this dissociation energy. The three-body channels are S<sub>2</sub> + H + isobutene, S<sub>2</sub> + CH<sub>3</sub> + propene, and S + SH + isobutene. The first two of these channels result from a sequential dissociation process in which loss of S<sub>2</sub> from <i>t</i>-BuSS results in ground state <i>t</i>-Bu with sufficient internal energy to undergo secondary fragmentation. The third three-body channel, S + SH + isobutene, is attributed to loss of internally excited HS<sub>2</sub> from <i>t</i>-BuSS, which then rapidly dissociates to form S + SH in an asynchronous concerted dissociation process. </p>


1989 ◽  
Vol 91 (12) ◽  
pp. 7498-7513 ◽  
Author(s):  
Karen A. Trentelman ◽  
Scott H. Kable ◽  
David B. Moss ◽  
Paul L. Houston

2020 ◽  
Author(s):  
Bethan Nichols ◽  
Erin Sullivan ◽  
Daniel Neumark

<p>The photodissociation dynamics of the <i>tert</i>-butyl perthiyl (<i>t</i>-BuSS) radical are investigated by fast-beam coincidence translational spectroscopy. A fast (6-8 keV) beam of neutral <i>t</i>-BuSS radicals is produced via photodetachment of the corresponding anion, followed by photodissociation at 248 nm (5.00 eV) or 193 nm (6.42 eV) and coincident detection of the neutral products. Photofragment mass and translational energy distributions are obtained at both wavelengths. At 248 nm, the dominant product channel (90%) is found to be S loss, with a product translational energy distribution that peaks close to the maximum available energy and an anisotropic photofragment angular distribution, indicating dissociation along a repulsive excited state. A minor channel (10%) leading to the formation of S<sub>2</sub> + <i>t</i>-Bu is also observed. At 193 nm, both two- and three-body dissociation are observed. Formation of S<sub>2</sub> + <i>t</i>-Bu is the dominant two-body product channel, with multiple electronic states of the S<sub>2</sub> molecule produced via excited state dissociation processes. Formation of S + <i>t</i>-BuS is a minor two-body channel at this dissociation energy. The three-body channels are S<sub>2</sub> + H + isobutene, S<sub>2</sub> + CH<sub>3</sub> + propene, and S + SH + isobutene. The first two of these channels result from a sequential dissociation process in which loss of S<sub>2</sub> from <i>t</i>-BuSS results in ground state <i>t</i>-Bu with sufficient internal energy to undergo secondary fragmentation. The third three-body channel, S + SH + isobutene, is attributed to loss of internally excited HS<sub>2</sub> from <i>t</i>-BuSS, which then rapidly dissociates to form S + SH in an asynchronous concerted dissociation process. </p>


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