Dipole—Quadrupole and Retardation Effects in Low‐Energy Atom—Atom Scattering
dc.contributor.author | Fontana, Peter R. | en_US |
dc.contributor.author | Bernstein, Richard B. | en_US |
dc.date.accessioned | 2010-05-06T20:55:26Z | |
dc.date.available | 2010-05-06T20:55:26Z | |
dc.date.issued | 1964-09-01 | en_US |
dc.identifier.citation | Fontana, Peter R.; Bernstein, Richard B. (1964). "Dipole—Quadrupole and Retardation Effects in Low‐Energy Atom—Atom Scattering." The Journal of Chemical Physics 41(5): 1431-1434. <http://hdl.handle.net/2027.42/69647> | en_US |
dc.identifier.uri | https://hdl.handle.net/2027.42/69647 | |
dc.description.abstract | Simple approximation formulas are derived for the dipole—quadrupole and retardation effects upon the total elastic scattering cross section for atomic collisions in the thermal energy range. For a long‐range potential containing both the dipole—dipole and dipole—quadrupole terms, i.e., V(r) = —(C(6)/r6)[1+(β/r2)], one finds ΔQ/QMM≈⅔π(β/QMM) where QMM is the Massey—Mohr cross section for an inverse sixth‐power attraction. For a long‐range potential including dipole—dipole and retardation effects, approximated by V(r) = —(C(6)/r6)[a/(a+r)], one obtains ΔQ/QMM ≈ −(QMM½)/aΔQ∕QMM≈−(π−32QMM12)∕a. Since these deviations are small and opposite in sign, it is concluded that the contributions of the dipole—quadrupole and retardation effects to the total cross sections are not sufficient to account for any significant discrepancy between theoretical and experimental Q values. | en_US |
dc.format.extent | 3102 bytes | |
dc.format.extent | 261540 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 | Dipole—Quadrupole and Retardation Effects in Low‐Energy Atom—Atom Scattering | 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 | Physics Department, University of Michigan, Ann Arbor, Michigan | en_US |
dc.contributor.affiliationother | Theoretical Chemistry Institute and Chemistry Department, University of Wisconsin, Madison, Wisconsin | en_US |
dc.description.bitstreamurl | http://deepblue.lib.umich.edu/bitstream/2027.42/69647/2/JCPSA6-41-5-1431-1.pdf | |
dc.identifier.doi | 10.1063/1.1726085 | en_US |
dc.identifier.source | The Journal of Chemical Physics | en_US |
dc.identifier.citedreference | H. S. W. Massey and C. B. O. Mohr, Proc. Roy. Soc. (London) A144, 188 (1934). | en_US |
dc.identifier.citedreference | R. B. Bernstein, Proceedings of the Third International Conference on the Physics of Electronic and A tomic Collisions, London, 1963 (North Holland Publishing Company, Amsterdam, to be published). | en_US |
dc.identifier.citedreference | E. W. Rothe and R. B. Bernstein, J. Chem. Phys. 31, 1619 (1959). | en_US |
dc.identifier.citedreference | H. Pauly, Fortsch. Physik 9, 613 (1961). | en_US |
dc.identifier.citedreference | A. Dalgarno, Rev. Mod. Phys. 35, 611 (1963); also Refs. 2–4. | en_US |
dc.identifier.citedreference | R. B. Bernstein and K. H. Kramer, J. Chem. Phys. 38, 2507 (1963). | en_US |
dc.identifier.citedreference | J. F. Hornig and J. O. Hirschfelder, J. Chem. Phys. 20, 1812 (1952); P. R. Fontana, Phys. Rev. 123, 1865 (1961). | en_US |
dc.identifier.citedreference | R. B. Bernstein, J. Chem. Phys. 38, 515 (1963). | en_US |
dc.identifier.citedreference | E. W. Rothe, P. K. Rol, S. M. Trujillo, and R. H. Neynaber, Phys. Rev. 128, 659 (1962). | en_US |
dc.identifier.citedreference | J. C. Kirkwood, Physik Z. 33, 57 (1932); A. Müller, Proc. Roy. Soc. (London) A154, 624 (1936). | en_US |
dc.identifier.citedreference | A. B. G. Casimir and D. Polder, Phys. Rev. 73, 360 (1948). | en_US |
dc.identifier.citedreference | P. R. Fontana, Ref. 2. | en_US |
dc.owningcollname | Physics, Department of |
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