2009
DOI: 10.1021/jp908934j
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Full State-Resolved Energy Gain Profiles of CO2 (J = 2−80) from Collisions of Highly Vibrationally Excited Molecules. 1. Relaxation of Pyrazine (E = 37900 cm−1)

Abstract: State-resolved energy gain profiles for "strong" and "weak" collisions of pyrazine (E = 37900 cm(-1)) and CO(2) are reported. Nascent energy profiles for scattered CO(2) (00(0)0, J = 2-64) were measured using high-resolution transient IR absorption spectroscopy at lambda = 2.7 microm. The data are combined with earlier data for CO(2) (J = 58-80) to yield the full state-resolved distribution of scattered CO(2) (00(0)0). The scattered CO(2) (00(0)0, J = 2-80) molecules have a biexponential rotational distributio… Show more

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Cited by 19 publications
(24 citation statements)
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“…Efficiency of our approach is achieved by simultaneous weighted sampling of several quasi-classical parameters of the system: impact parameter of the quencher, its incident direction, thermal energy of the molecule + quencher collisions and, finally, the distribution of initial rotational states of the energized molecule. The procedure is general and can be applied to many processes relevant to combustion, 66 astrochemistry, 67 and atmospheric chemistry. 68 Second, we applied this method to address a longstanding problem -the recombination reaction that forms ozone.…”
Section: Discussionmentioning
confidence: 99%
“…Efficiency of our approach is achieved by simultaneous weighted sampling of several quasi-classical parameters of the system: impact parameter of the quencher, its incident direction, thermal energy of the molecule + quencher collisions and, finally, the distribution of initial rotational states of the energized molecule. The procedure is general and can be applied to many processes relevant to combustion, 66 astrochemistry, 67 and atmospheric chemistry. 68 Second, we applied this method to address a longstanding problem -the recombination reaction that forms ozone.…”
Section: Discussionmentioning
confidence: 99%
“…On the other side, we can work with the fluid rotor equations and substitute (13 ), (20), and (21) into (14 ). This leads to the matrix equation given in Appendix A.…”
Section: B Equivalence Of the Two Methodsmentioning
confidence: 99%
“…In recent years, the interest in collisional energy transfer at ultra-cold conditions has been high [14][15][16] and in those cases the inelastic scattering calculations must be done using the full-fledged quantum mechanics. 17,18 On the other hand, for the processes relevant to combustion, 19,20 photochemistry, 21,22 or hyper-thermal phenomena, 23,24 when high energies are involved, the classical-trajectory picture is quite appropriate. [25][26][27][28][29] In between those limits, the quantum mechanical calculations of collisional energy transfer become unaffordable computationally even for the smallest molecular systems (due to a large number of coupled channels and partial waves) while the classical trajectory calculations are not entirely justified and contain serious drawbacks (such as a) Author to whom correspondence should be addressed.…”
Section: Introductionmentioning
confidence: 99%
“…There have been numerous studies on CET between highly vibrationally excited polyatomic molecules and various bath gases. Previous studies include highly vibrationally excited benzene, [1][2][3] deuterated and halogenated benzenes, 1,[3][4][5][6][7] alkyl benzenes, 8 azulene, 9 naphthalene, 10 cycloheptatrienes, 11 and pyrazine 12 in a range of atomic and molecular baths including noble gases, 1 CO 2 , [3][4][5]12,13 N 2 , 6,7 and H 2 O. 14 The photophysics of highly vibrationally excited benzene has been the subject of numerous studies.…”
Section: Introductionmentioning
confidence: 99%