Probing the effect of the H2 rotational state in O(1D)+H2→OH+H:: Theoretical dynamics including nonadiabatic effects and a crossed molecular beam study

被引:90
作者
Gray, SK [1 ]
Balint-Kurti, GG
Schatz, GC
Lin, JJ
Liu, XH
Harich, S
Yang, XM
机构
[1] Argonne Natl Lab, Div Chem, 9700 S Cass Ave, Argonne, IL 60439 USA
[2] Univ Bristol, Sch Chem, Bristol B58 1TS, Avon, England
[3] Northwestern Univ, Dept Chem, Evanston, IL 60208 USA
[4] Acad Sinica, Inst Atom & Mol Sci, Taipei 10764, Taiwan
[5] Natl Tsing Hua Univ, Dept Chem, Hsinchu, Taiwan
关键词
D O I
10.1063/1.1313785
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
Theoretical estimates of reactive cross sections for O(D-1)+H-2(X,upsilon =0,j)--> OH(X)+H(S-2), with H-2 rotational quantum numbers j=0 and 1, are obtained for a range of collision energies, E-col. Crossed molecular beam measurements are also used to infer the ratio, r(1,0), of the j=1 and 0 cross sections at E-col=0.056 eV. The theory indicates that the 1 (1)A' potential surface is the most important one. However, the 2 (1)A' and 1 (1)A' surfaces can also contribute. Adiabatic dynamics on the 1 (1)A' surface, particularly at E-col above its 0.1 eV barrier to reaction plays a role. The 2 (1)A' surface, while not correlating with ground electronic state products, can still lead to products via nonadiabatic interactions with the 1 (1)A' surface. Many quantum dynamics and quasiclassical classical trajectory calculations are carried out. Accurate, ab initio based potential energy surfaces are employed. Quantum cross sections are based on helicity decoupled wave packet calculations for several values of total angular momentum. Nonadiabatic wave packet and trajectory surface hopping calculations, where appropriate, are carried out. An interesting, subtle picture emerges regarding the energy dependence of r(1,0). The theoretical results indicate, somewhat surprisingly, that, for E-col<0.1 eV,r(1,0) can be less than unity owing to the anisotropy of the ground state potential. Electronically excited states and nonadiabatic effects contribute to the overall cross sections for E-col>0.1 eV, but the full r(1,0) is only weakly sensitive to excited states. Our experimentally inferred r(1,0) at E-col=0.056 eV, 0.95 +/-0.02, is in quantitative agreement with our best calculation, which suggests that the effect of potential anisotropy is correctly described by theory. The relation between these results and previous experimental findings is discussed. (C) 2000 American Institute of Physics. [S0021-9606(00)02041-9].
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页码:7330 / 7344
页数:15
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