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Extrema in Velocity Dependence of Total Elastic Cross Sections for Atomic Beam Scattering: Relation to Di‐atom Bound States

dc.contributor.authorBernstein, Richard B.en_US
dc.date.accessioned2010-05-06T22:22:03Z
dc.date.available2010-05-06T22:22:03Z
dc.date.issued1962-10-15en_US
dc.identifier.citationBernstein, Richard B. (1962). "Extrema in Velocity Dependence of Total Elastic Cross Sections for Atomic Beam Scattering: Relation to Di‐atom Bound States." The Journal of Chemical Physics 37(8): 1880-1881. <http://hdl.handle.net/2027.42/70569>en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/70569
dc.format.extent3102 bytes
dc.format.extent168009 bytes
dc.format.mimetypetext/plain
dc.format.mimetypeapplication/pdf
dc.publisherThe American Institute of Physicsen_US
dc.rights© The American Institute of Physicsen_US
dc.titleExtrema in Velocity Dependence of Total Elastic Cross Sections for Atomic Beam Scattering: Relation to Di‐atom Bound Statesen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumChemistry Department, University of Michigan, Ann Arbor, Michiganen_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/70569/2/JCPSA6-37-8-1880-1.pdf
dc.identifier.doi10.1063/1.1733383en_US
dc.identifier.sourceThe Journal of Chemical Physicsen_US
dc.identifier.citedreferenceR. B. Bernstein, J. Chem. Phys. 34, 361 (1961); 33, 795 (1960).en_US
dc.identifier.citedreferenceE. W. Rothe, P. K. Rol, S. M. Trujillo, and R. H. Neynaber, Phys. Rev. (to be published).en_US
dc.identifier.citedreferenceFor simplicity we limit consideration to unlike atom collisions involving one 1S01S0 state atom (Group II or VIII) and one either 1S01S0 or 2S½2S12 (Group I), yielding the single molecular state 1Σ+1Σ+ or 2Σ+.2Σ+.en_US
dc.identifier.citedreferenceR. B. Bernstein, J. Chem. Phys. 36, 1403 (1962).en_US
dc.identifier.citedreferenceIt has not been possible to prove this in general, however. Thus in unfavorable circumstances it is possible that M  =  n+1.M=n+1.en_US
dc.identifier.citedreferenceSee P. Swan, Proc. Roy. Soc. (London) A228, 10 (1955); in the present case3 Pauli excluded states are not involved.en_US
dc.owningcollnamePhysics, Department of


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