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Journal of the Optical Society of America

Journal of the Optical Society of America

  • Vol. 64, Iss. 12 — Dec. 1, 1974
  • pp: 1722–1723

Models for the Goos—Haenchen effect

A. Kodre and J. Strnad  »View Author Affiliations


JOSA, Vol. 64, Issue 12, pp. 1722-1723 (1974)
http://dx.doi.org/10.1364/JOSA.64.001722


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Citation
A. Kodre and J. Strnad, "Models for the Goos—Haenchen effect," J. Opt. Soc. Am. 64, 1722-1723 (1974)
http://www.opticsinfobase.org/josa/abstract.cfm?URI=josa-64-12-1722


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References

  1. F. Goos and L. Haenchen, Ann. Physik 1, 333 (1947); Ann. Physik 5, 251 (1949).
  2. H. Wolter, Z. Naturforschg. 5a, 143 (1950).
  3. A. Mazet, Ch. Imbert, and S. Huard, Compt. Rend. B 273, 592 (1971).
  4. Ch. Imbert, Phys. Rev. D 5, 787 (1972).
  5. R. H. Renard, J. Opt. Soc. Am. 54, 1190 (1964).
  6. H. K. V. Lotsch, J. Opt. Soc. Am. 58, 551 (1968). This paper contains an extensive list of references.
  7. M. Ricard, Nouv. Rev. d'Optique 4, 63 (1973).
  8. J. L. Agudin, Phys. Rev. 171, 1358 (1968). Agudin's calculation is considered the best quantum analysis of the Goos—Haenchen effect (L. de Broglie and J. P. Vigier, Phys. Rev. Lett. 28, 1001 (1972)).
  9. E. P. Wigner, Phys. Rev. 98, 145 (1955), F. T. Smith, Phys. Rev. 118, 349 (1960), M. Froissart, M. L. Goldberger, and K. M. Watson, Phys. Rev. 131, 2820 (1963).
  10. In the limit of the critical angle, all models produce equal results. At grazing incidence (Φ1 → ½π) the shift XE and the delay time tE tend to zero, whereas xM = xS and tM = tS become infinite. This behavior has been often used against the marked-wave method. However, the results of the stationary-phase method and of scattering theory exhibit the same feature.

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