Collisional energy transfer in highly vibrationally excited H2CO(
1A1)
J. Chem. Phys. 87, 1895 (1987); doi:10.1063/1.453207
Issue Date: 1 August 1987
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Collisional energy transfer has been investigated in highly vibrationally excited H2CO (
1A1) at Evib
11 400 cm−1 using the method of stimulated emission pumping–transient absorption spectroscopy (SEP-TAS). Total depopulation and state-to-state rate constants were measured for several rotational levels of the 2444 vibrational state. For H2CO self-relaxation the depopulation rate constant of the 61,5 level was measured to be k0=(3.12±0.13)×10−9 cm3/molecule s. An analysis of the state-to-state data with a simplified master equation approach yielded rate constants k1=(7.7±1.2)×10−10, k2=(1.2±0.3)×10−10, and k3=(0.6±0.3)×10−10 cm3/molecule s for collisions with
J=1, 2, and 3, respectively, and
Ka=0,
Kc=
J, the reverse rate constants being given by microscopic reversibility. Thus, the
J=±1 steps account for ~50% of all inelastic collisions, which can be rationalized in terms of a simple dipole–dipole interaction. At Evib
11 400 cm−1, where
vib
0.42/cm−1, collisions seem to conserve the vibrational character in spite of the fact that the energy gap between adjacent vibrational states is a fraction of the transferred rotational energy.
The Journal of Chemical Physics is copyrighted by The American Institute of Physics.
11 400 cm−1 using the method of stimulated emission pumping–transient absorption spectroscopy (SEP-TAS). Total depopulation and state-to-state rate constants were measured for several rotational levels of the 2444 vibrational state. For H2CO self-relaxation the depopulation rate constant of the 61,5 level was measured to be k0=(3.12±0.13)×10−9 cm3/molecule s. An analysis of the state-to-state data with a simplified master equation approach yielded rate constants k1=(7.7±1.2)×10−10, k2=(1.2±0.3)×10−10, and k3=(0.6±0.3)×10−10 cm3/molecule s for collisions with
J=1, 2, and 3, respectively, and
Ka=0,
Kc=
J, the reverse rate constants being given by microscopic reversibility. Thus, the
J=±1 steps account for ~50% of all inelastic collisions, which can be rationalized in terms of a simple dipole–dipole interaction. At Evib
11 400 cm−1, where
vib
0.42/cm−1, collisions seem to conserve the vibrational character in spite of the fact that the energy gap between adjacent vibrational states is a fraction of the transferred rotational energy.
The Journal of Chemical Physics is copyrighted by The American Institute of Physics.
| History: | Received 21 April 1987; accepted 26 May 1987 |
| Permalink: |
http://link.aip.org/link/?JCPSA6/87/1895/1 |
KEYWORDS and PACS
FORMALDEHYDE,
VIBRATIONAL STATES,
ENERGY TRANSFER,
EXCITED STATES,
LASER SPECTROSCOPY,
RELAXATION,
KINETICS,
MOLECULE&minus,
MOLECULE COLLISIONS,
ABSORPTION SPECTRA
- 34.50.Ez
Atomic and molecular collision processes and interactions Inelastic scattering of atoms and molecules Rotational and vibrational energy transfer - 33.20.Kf
Molecular spectra and interactions of molecules with photons Molecular spectra, grouped by wavelength ranges Visible spectra - 33.20.Lg
Molecular spectra and interactions of molecules with photons Molecular spectra, grouped by wavelength ranges Ultraviolet spectra - 34.50.Pi
Atomic and molecular collision processes and interactions Inelastic scattering of atoms and molecules State-to-state scattering analyses - YEAR: 1987
RELATED DATABASES
PUBLICATION DATA
0021-9606 (print)
1089-7690 (online)
REFERENCES (14)
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