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Electron diffraction studies of laser‐pumped molecules. IV. SF6, experiment and theory

dc.contributor.authorBartell, Lawrence S.en_US
dc.contributor.authorKacner, Michael A.en_US
dc.date.accessioned2010-05-06T21:22:46Z
dc.date.available2010-05-06T21:22:46Z
dc.date.issued1984-07-01en_US
dc.identifier.citationBartell, Lawrence S.; Kacner, Michael A. (1984). "Electron diffraction studies of laser‐pumped molecules. IV. SF6, experiment and theory." The Journal of Chemical Physics 81(1): 280-287. <http://hdl.handle.net/2027.42/69936>en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/69936
dc.description.abstractA model of absorption of infrared radiation by supersonic jets proposed in paper III was tested experimentally. New nozzle designs permitted pumping the ν3 mode of SF6 at power densities in excess of 104 W/cm2. Vibrational excitation corresponding to the absorption of up to 3.6 photons/molecule was deduced from the increased amplitudes of vibration of the SF, FFcis, and FFtrans atom pairs and the lengthening of the SF bond. At high excitations, electron diffraction intensities were accounted for best if it was assumed that two subsets of molecules were produced, one much hotter than the other. Vibration–vibration relaxation from ν3 to the other stretching modes was too fast to be followed. Relaxation of stretching to bending could be monitored, crudely, at lower pressures where approximately 30 collisions were needed at the depressed temperatures in the jet. At higher pressures and excitations V‐T/R relaxation was observed, corresponding to a transfer of perhaps one‐tenth of the vibrational excitation in the course of 103 collisions. Excitation as a function of gas density, power density, and nozzle diameter was accounted for satisfactorily by the model of paper III.en_US
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dc.publisherThe American Institute of Physicsen_US
dc.rights© The American Institute of Physicsen_US
dc.titleElectron diffraction studies of laser‐pumped molecules. IV. SF6, experiment and theoryen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumDepartment of Chemistry, University of Michigan, Ann Arbor, Michigan 48109en_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/69936/2/JCPSA6-81-1-280-1.pdf
dc.identifier.doi10.1063/1.447382en_US
dc.identifier.sourceThe Journal of Chemical Physicsen_US
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dc.identifier.citedreferenceSee AIP document No. PAPS JCPSA‐81‐280‐18 for 18 pages of experimental conditions for all diffraction plates, analyses of the plates, representative experimental intensities, and the nozzles as a function of stagnation pressure. Order by PAPS number and journal reference from American Institute of Physics, Physics Auxilliary Publication Service, 335 E. 45 St., New York, NY 10017. The price is $1.50 for each microfiche (98 pages) or $5 for photocopies of up to 30 pages and $0.15 for each page over 30 pages. Airmail is additional. Make checks payable to the American Institute of Physics.en_US
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dc.identifier.citedreferenceInasmuch as the absorption takes place in the first nozzle diameter or so of the jet flow, it is only necessary that the breadth of the polished region responsible for reflections be large compared with the 102μ m102μm span of the jet orifice.en_US
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dc.owningcollnamePhysics, Department of


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