Reaction pathway and energy disposal of the CaH product in the reaction of Ca(4s4p 1P1)+CH4→CaH(X 2Σ+)+CH3

被引:5
|
作者
Chen, JJ
Song, YW
Lin, KC [1 ]
Hung, YM
机构
[1] Natl Taiwan Univ, Dept Chem, Taipei 10764, Taiwan
[2] Acad Sinica, Inst Atom & Mol Sci, Taipei 106, Taiwan
[3] Chinese Culture Univ, Dept Chem, Taipei 111, Taiwan
[4] Chinese Culture Univ, Inst Appl Chem, Taipei 111, Taiwan
来源
JOURNAL OF CHEMICAL PHYSICS | 2003年 / 118卷 / 11期
关键词
D O I
10.1063/1.1545107
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
The reaction pathway for Ca(4s4p P-1(1))+CH4-->CaH(X (2)Sigma(+))+CH3 has been investigated by using the pump-probe technique in combination with potential energy surface (PES) calculations. The nascent product distributions of CaH have been found with a Boltzmann rotational temperature of 988+/-66 and 864+/-75 K for the v=0 and 1 levels, respectively, and a Boltzmann vibrational temperature of 1960+/-80 K. The rotational and vibrational energy partitions in CaH have been estimated to be 555+/-22 and 995+/-10 cm-1, respectively. According to the PES calculations, the pathway is found to favor an insertion mechanism. Ca(4 P-1(1)) approaches CH4 in C-2v or C-s symmetry and then the collision complex may undergo a series of surface transitions to the ground state surface with which the products correlate. The findings of low rotation and high vibration for CaH may be interpreted from two aspects. First, the Ca-C bond distance of the intermediate around the surface crossing region is 2.7-2.8 Angstrom, close to the equilibrium bond distance 2.349 Angstrom. The strong coupling of the moieties renders the energy transfer sufficient from CaH into the CH3 radical. Second, after the 2A(')-1 A(') surface transition, the HCaCH3 intermediate with a small excess energy may be energetically stabilized. The long-lived collision complex may have enough time for energy randomization prior to flying apart. (C) 2003 American Institute of Physics.
引用
收藏
页码:4938 / 4944
页数:7
相关论文
共 50 条
  • [21] PREPARATION OF LIA1[P(CH3)2]4 AND SILYLPHOSPHINES H3-X(CH3)XSI-P(CH3)2
    FRITZ, G
    SCHAFER, H
    [J]. ZEITSCHRIFT FUR ANORGANISCHE UND ALLGEMEINE CHEMIE, 1974, 406 (2-3): : 167 - 170
  • [22] QUENCHING OF BA(1P1) BY CH4 MOLECULES WITHIN ARGON CLUSTERS
    LALLEMENT, A
    SUBLEMONTIER, O
    VISTICOT, JP
    BELL, AJ
    BERLANDE, J
    CUVELLIER, J
    MESTDAGH, JM
    MEYNADIER, P
    [J]. CHEMICAL PHYSICS LETTERS, 1993, 204 (5-6) : 440 - 444
  • [24] Direct Dynamics Study on CH2O + CH3~·→ CHO + CH4 Reaction
    Yan QI
    [J]. Chinese Chemical Letters, 2006, (04) : 565 - 568
  • [25] Ab initio ground potential energy surface, VTST and QCT study of the O(3P)+CH4(X1A1)→OH(X2Π)+CH3(X2A2") reaction
    González, M
    Hernando, J
    Millán, J
    Sayós, R
    [J]. JOURNAL OF CHEMICAL PHYSICS, 1999, 110 (15): : 7326 - 7338
  • [26] REACTION-PATH DYNAMICS OF CL + CH4 -] HCL + CH3
    TRUONG, TN
    JOSEPH, T
    MELISSAS, V
    TRUHLAR, DG
    [J]. ABSTRACTS OF PAPERS OF THE AMERICAN CHEMICAL SOCIETY, 1989, 197 : 90 - PHYS
  • [27] The effect of the symmetric and asymmetric stretching vibrations of CH4 on the O(3P)+CH4→OH+CH3 reaction
    Palma, J
    Clary, DC
    [J]. PHYSICAL CHEMISTRY CHEMICAL PHYSICS, 2000, 2 (18) : 4105 - 4114
  • [28] Accurate quantum dynamics of a combustion reaction:: Thermal rate constants of O(3P)+CH4(X1A1)→OH(X2Π)+CH3(X2A2")
    Huarte-Larrañaga, F
    Manthe, U
    [J]. JOURNAL OF CHEMICAL PHYSICS, 2002, 117 (10): : 4635 - 4638
  • [29] Accurate ab initio potential energy surface, thermochemistry, and dynamics of the Br(2P, 2P3/2) + CH4 → HBr + CH3 reaction
    Czako, Gabor
    [J]. JOURNAL OF CHEMICAL PHYSICS, 2013, 138 (13):
  • [30] Reaction dynamics of the Ca(D-1(2), P-3(J))+CH3I->CaI*+CH3 system: chemiluminescence, energy disposal and product polarization
    Orea, JM
    Laplaza, A
    Rinaldi, CA
    Tardajos, G
    Urena, AG
    [J]. CHEMICAL PHYSICS, 1997, 220 (03) : 337 - 354