The roaming atom pathway in formaldehyde decomposition

被引:81
作者
Lahankar, Sridhar A.
Chambreau, Steven D.
Townsend, Dave
Suits, Frank
Farnum, John
Zhang, Xiubin
Bowman, Joel M.
Suits, Arthur G. [1 ]
机构
[1] Wayne State Univ, Dept Chem, Detroit, MI 48202 USA
[2] IBM Corp, TJ Watson Res Ctr, Computat Biol Ctr, Yorktown Hts, NY 10598 USA
[3] Emory Univ, Dept Chem, Atlanta, GA 30322 USA
[4] Emory Univ, Cherry L Emerson Ctr Sci Computat, Atlanta, GA 30322 USA
关键词
D O I
10.1063/1.2202241
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
We present a detailed experimental and theoretical investigation of formaldehyde photodissociation to H-2 and CO following excitation to the 2(1)4(1) and 2(1)4(3) transitions in S-1. The CO velocity distributions were obtained using dc slice imaging of single CO rotational states (v=0, j(CO)=5-45). These high-resolution measurements reveal the correlated internal state distribution in the H-2 cofragments. The results show that rotationally hot CO (j(CO)similar to 45) is produced in conjunction with vibrationally "cold" H-2 fragments (v=0-5): these products are formed through the well-known skewed transition state and described in detail in the accompanying paper. After excitation of formaldehyde above the threshold for the radical channel (H2CO -> H+HCO) we also find formation of rotationally cold CO (j(CO)=5-28) correlated to highly vibrationally excited H-2 (v=6-8). These products are formed through a novel mechanism that involves near dissociation followed by intramolecular H abstraction [D. Townsend , Science 306, 1158 (2004)], and that avoids the region of the transition state entirely. The dynamics of this "roaming" mechanism are the focus of this paper. The correlations between the vibrational states of H-2 and rotational states of CO formed following excitation on the 2(1)4(3) transition allow us to determine the relative contribution to molecular products from the roaming atom channel versus the conventional molecular channel. (c) 2006 American Institute of Physics.
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页数:10
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