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General Form of the Retarded van der Waals Potential

J. Chem. Phys. 48, 3333 (1968); doi:10.1063/1.1669611

Issue Date: 1 April 1968

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G. Feinberg
Department of Physics, Columbia University, New York, New York

J. Sucher
Center for Theoretical Physics, Department of Physics and Astronomy, University of Maryland, College Park, Maryland

Abstract not available.

©1968 American Institute of Physics
History: Received 22 December 1967
Permalink: http://link.aip.org/link/?JCPSA6/48/3333/1
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ISSN:
0021-9606 (print)   1089-7690 (online)
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REFERENCES (7)

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  1. H. B. G. Casimir and D. Polder, Phys. Rev. 73, 360 (1948).
  2. For a very recent review of these methods, see E. A. Power, Advan. Chem. Phys. 12, 167 (1967).
  3. See also the list of references in W. J. Meath and J. O. Hirschfelder, J. Chem. Phys. 44, 3210 (1966).
  4. G. Feinberg and J. Sucher, Phys. Rev. 139, B1619 (1965).
  5. J. Softer and J. Sucher, Phys. Rev. 161, 1664 (1967).
  6. A result similar to our Eq. (1) occurs in the work of C. Mavroyannis and M. J. Stephen, Mol. Phys. 5, 629 (1962).
  7. However, these authors have only included the contribution to the magnetic polarizability coming from orbital magnetic moments, omitting the spin moments and the diagmagnetic terms. Hence what is effectively their expression for alphaM is seriously inadequate for most systems, in particular for hydrogen atoms.
  8. See, e.g., J. H. Van Vleck, Electric and Magnetic Susceptibilities (Oxford University Press, London, 1931).
  9. G. Breit and I. I. Rabi, Phys. Rev. 38, 2082 (1931).
  10. For a discussion of measurements of the retarded van der Waals attraction, see B. V. Deriagin and I. I. Abrikosova, Sov. Phys.—JETP 3, 819 (1957)
  11. [Zh. Eksp. Teor. Fiz. 3, 993 (1956)].

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