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Journal of the Optical Society of America

Journal of the Optical Society of America

  • Vol. 72, Iss. 3 — Mar. 1, 1982
  • pp: 327–330

Holography and the inverse source problem

R. P. Porter and A. J. Devaney  »View Author Affiliations


JOSA, Vol. 72, Issue 3, pp. 327-330 (1982)
http://dx.doi.org/10.1364/JOSA.72.000327


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Abstract

The inverse source problem for monochromatic sources Re[ρ(r, ω)e-iωt] to the scalar-wave equation is investigated. It is shown that a unique solution to the inverse source problem can be obtained by imposing the constraint that the solution minimize the source energy E = ∫ d3r|ρ(r, ω)|2. For certain recording geometries the time derivative of the real image produced by a point-reference hologram is shown to be directly proportional to the time-reversed minimum energy source Re[ρ*ME(r, ω)e-iωt] in the short-wavelength limit.

© 1982 Optical Society of America

Citation
R. P. Porter and A. J. Devaney, "Holography and the inverse source problem," J. Opt. Soc. Am. 72, 327-330 (1982)
http://www.opticsinfobase.org/josa/abstract.cfm?URI=josa-72-3-327


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References

  1. A. Sommerfeld, Partial Differential Equations in Physics (Academic, New York, 1967), p. 189.
  2. R. P. Porter, "Diffraction-limited, scalar image formation with holograms of arbitrary shape," J. Opt. Soc. Am. 60, 1051–1059 (1970); "Image formation with arbitrary holographic type surfaces," Phys. Lett. 29A, 193–194 (1969).
  3. N. N. Bojarski, "Inverse Scattering," Naval Air Systems Command Rep., contract N00019-73-C-0312, (Naval Air Systems Command, Washington, D.C., 1973), Sec. 11, pp. 3–6. The form of Bojarski's integral equation employed in this paper is that given in Ref. 5.
  4. A. J. Devaney and E. Wolf, "Radiating and nonradiating classical current distributions and the fields they generate," Phys. Rev. D 8, 1044–1047 (1973).
  5. N. Bleistein and J. Cohen, "Nonuniqueness in the inverse source problem in acoustics and electromagnetics," J. Math. Phys. 18, 194–201 (1977).
  6. A. J. Devaney and G. C. Sherman, "Nonuniqueness in inverse source and scattering problems," IEEE Trans. Antennas Propag. (to be published).
  7. We use the definitions of the spherical harmonics and spherical Bessel and Hankel functions employed by A. Messiah, Quantum Mechanics (North-Holland, Amsterdam, 1965), Vol. I, Apps. BII and BIV.
  8. M. Abramowitz and I. A. Stegun, eds., Handbook of Mathematical Functions (Dover, New York, 1972), p. 440.
  9. K. Gottfried, Quantum Mechanics (Benjamin, New York, 1966), p. 90.
  10. For a discussion on time reversal in holography see W. Lukosz, "Equivalent-lens theory of holographic imaging," J. Opt. Soc. Am. 58, 1084–1091 (1968).

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