Communication: Experimental and theoretical investigations of the effects of the reactant bending excitations in the F+CHD3 reaction
被引:47
作者:
Czako, Gabor
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Emory Univ, Dept Chem, Atlanta, GA 30322 USA
Emory Univ, Cherry L Emerson Ctr Sci Computat, Atlanta, GA 30322 USAEmory Univ, Dept Chem, Atlanta, GA 30322 USA
Czako, Gabor
[1
,2
]
Shuai, Quan
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机构:
Acad Sinica, IAMS, Taipei 10617, Taiwan
Chinese Acad Sci, Dalian Inst Chem Phys, State Key Lab Mol React Dynam, Dalian 116023, Peoples R ChinaEmory Univ, Dept Chem, Atlanta, GA 30322 USA
Shuai, Quan
[3
,4
]
Liu, Kopin
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机构:
Acad Sinica, IAMS, Taipei 10617, TaiwanEmory Univ, Dept Chem, Atlanta, GA 30322 USA
Liu, Kopin
[3
]
Bowman, Joel M.
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机构:
Emory Univ, Dept Chem, Atlanta, GA 30322 USA
Emory Univ, Cherry L Emerson Ctr Sci Computat, Atlanta, GA 30322 USAEmory Univ, Dept Chem, Atlanta, GA 30322 USA
Bowman, Joel M.
[1
,2
]
机构:
[1] Emory Univ, Dept Chem, Atlanta, GA 30322 USA
[2] Emory Univ, Cherry L Emerson Ctr Sci Computat, Atlanta, GA 30322 USA
[3] Acad Sinica, IAMS, Taipei 10617, Taiwan
[4] Chinese Acad Sci, Dalian Inst Chem Phys, State Key Lab Mol React Dynam, Dalian 116023, Peoples R China
The effects of the reactant bending excitations in the F+CHD3 reaction are investigated by crossed molecular beam experiments and quasiclassical trajectory (QCT) calculations using a high-quality ab initio potential energy surface. The collision energy (E-c) dependence of the cross sections of the F+CHD3(nu(b)=0,1) reactions for the correlated product pairs HF(nu')+CD3(nu(2)= 0,1) and DF(nu')+CHD2(nu(4)=0,1) is obtained. Both experiment and theory show that the bending excitation activates the reaction at low E-c and begins to inactivate at higher E-c. The experimental F+CHD3(nu(b)=1) excitation functions display surprising peak features, especially for the HF(nu'=3)+CD3(nu(2)=0,1) channels, indicating reactive resonances (quantum effects), which cannot be captured by quasiclassical calculations. The reactant state-specific QCT calculations predict that the nu(5)(e) bending mode excitation is the most efficient to drive the reaction and the nu(6)(e) and v(5)(e) modes enhance the DF and HF channels, respectively. (C) 2010 American Institute of Physics. [doi:10.1063/1.3490795]