Relative Quenching Cross Sections in the Reaction of Hg(63P1) Atoms with Isotopic N2O Molecules
dc.contributor.author | Hoffman, Morton Z. | en_US |
dc.contributor.author | Bernstein, Richard B. | en_US |
dc.date.accessioned | 2010-05-06T21:16:12Z | |
dc.date.available | 2010-05-06T21:16:12Z | |
dc.date.issued | 1960-08 | en_US |
dc.identifier.citation | Hoffman, Morton Z.; Bernstein, Richard B. (1960). "Relative Quenching Cross Sections in the Reaction of Hg(63P1) Atoms with Isotopic N2O Molecules." The Journal of Chemical Physics 33(2): 526-529. <http://hdl.handle.net/2027.42/69865> | en_US |
dc.identifier.uri | https://hdl.handle.net/2027.42/69865 | |
dc.description.abstract | The N14/N15 and O16/O18 isotope effects in the Hg(63P1)‐photosensitized decomposition of nitrous oxide have been measured. Observed isotopic fractionation factors, S0 (interpreted in terms of ratios of rate constants for quenching by N14N14O16 vs N15N14O16, N14N15O16, and N14N14O18), are related to the ratio of isotopic quenching cross sections by the equation Q/Q*=S0(μ/μ*)☒, where μ and μ* are the collisional reduced masses for Hg and the light and heavy isotopic molecules, respectively. The quenching cross section ratio for N142O16/N142O18 was unity within the experimental uncertainty (±0.1%). The ratios for N14N14O16/N15N14O16 and N14N14O16/N14N15O16 differed from unity by +0.98 and +0.44%, respectively. The order of the quenching cross sections for the isotopic nitrous oxide molecules is thus: N15N14O16<N14N15O16<14N14O18≅N14N14O16. The implications of the present observations are briefly discussed. | en_US |
dc.format.extent | 3102 bytes | |
dc.format.extent | 300427 bytes | |
dc.format.mimetype | text/plain | |
dc.format.mimetype | application/pdf | |
dc.publisher | The American Institute of Physics | en_US |
dc.rights | © The American Institute of Physics | en_US |
dc.title | Relative Quenching Cross Sections in the Reaction of Hg(63P1) Atoms with Isotopic N2O Molecules | en_US |
dc.type | Article | en_US |
dc.subject.hlbsecondlevel | Physics | en_US |
dc.subject.hlbtoplevel | Science | en_US |
dc.description.peerreviewed | Peer Reviewed | en_US |
dc.contributor.affiliationum | Department of Chemistry, The University of Michigan, Ann Arbor, Michigan | en_US |
dc.description.bitstreamurl | http://deepblue.lib.umich.edu/bitstream/2027.42/69865/2/JCPSA6-33-2-526-1.pdf | |
dc.identifier.doi | 10.1063/1.1731178 | en_US |
dc.identifier.source | The Journal of Chemical Physics | en_US |
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dc.identifier.citedreference | In the case of NN15O,NN15O, for example, the 4.3 at. %N15%N15 would be distributed as follows, in terms of all the molecules: N15NO = 0.4%,N15NO=0.4%, NN15O = 3.9%,NN15O=3.9%, and NNO = 95.7%.NNO=95.7%. | en_US |
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dc.identifier.citedreference | The symbols N and N∗ represent N14N14 and N15,N15, respectively, while O and O∗ refer, respectively, to O16O16 and O18.O18. | en_US |
dc.identifier.citedreference | The value of Y for sample A is: Y = (0.004)/(0.004+0.039) = 0.093;Y=(0.004)∕(0.004+0.039)=0.093; for sample B, Y = (0.039)/(0.039+0.004) = 0.907.Y=(0.039)∕(0.039+0.004)=0.907. | en_US |
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dc.owningcollname | Physics, Department of |
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