Abstract

Real-time interference fringes have been observed with a diffusely reflecting object in a holographic setup even when the photographic plate is exposed and viewed with the reference beam blanked off. Linear theory can account for these fringes if the major part of the object remains unchanged.

© 1978 Optical Society of America

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References

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  1. E. Marom, J. Katz, “Unconventional interferometric realizations based on holographic nonlinear effects,” Appl. Opt. 16, 1400 (1977).
    [Crossref] [PubMed]
  2. P. Hariharan, “Statistics of speckle patterns produced by a rough metal surface,” Opt. Acta 24, 979 (1977).
    [Crossref]
  3. R. J. Collier, K. S. Pennington, “Ghost imaging by holograms formed in the near field,” Appl. Phys. Lett. 8, 44 (1966).
    [Crossref]
  4. G. W. Stroke, R. Restrick, A. Funkhouser, D. Brumm, “Resolution-retrieving compensation of source effects by correlative reconstruction in high-resolution holography,” Phys. Lett. 18, 274 (1965).
    [Crossref]
  5. R. J. Collier, C. B. Burckhardt, L. H. Lin, Optical Holography (Academic, New York, 1971), p. 385.

1977 (2)

E. Marom, J. Katz, “Unconventional interferometric realizations based on holographic nonlinear effects,” Appl. Opt. 16, 1400 (1977).
[Crossref] [PubMed]

P. Hariharan, “Statistics of speckle patterns produced by a rough metal surface,” Opt. Acta 24, 979 (1977).
[Crossref]

1966 (1)

R. J. Collier, K. S. Pennington, “Ghost imaging by holograms formed in the near field,” Appl. Phys. Lett. 8, 44 (1966).
[Crossref]

1965 (1)

G. W. Stroke, R. Restrick, A. Funkhouser, D. Brumm, “Resolution-retrieving compensation of source effects by correlative reconstruction in high-resolution holography,” Phys. Lett. 18, 274 (1965).
[Crossref]

Brumm, D.

G. W. Stroke, R. Restrick, A. Funkhouser, D. Brumm, “Resolution-retrieving compensation of source effects by correlative reconstruction in high-resolution holography,” Phys. Lett. 18, 274 (1965).
[Crossref]

Burckhardt, C. B.

R. J. Collier, C. B. Burckhardt, L. H. Lin, Optical Holography (Academic, New York, 1971), p. 385.

Collier, R. J.

R. J. Collier, K. S. Pennington, “Ghost imaging by holograms formed in the near field,” Appl. Phys. Lett. 8, 44 (1966).
[Crossref]

R. J. Collier, C. B. Burckhardt, L. H. Lin, Optical Holography (Academic, New York, 1971), p. 385.

Funkhouser, A.

G. W. Stroke, R. Restrick, A. Funkhouser, D. Brumm, “Resolution-retrieving compensation of source effects by correlative reconstruction in high-resolution holography,” Phys. Lett. 18, 274 (1965).
[Crossref]

Hariharan, P.

P. Hariharan, “Statistics of speckle patterns produced by a rough metal surface,” Opt. Acta 24, 979 (1977).
[Crossref]

Katz, J.

Lin, L. H.

R. J. Collier, C. B. Burckhardt, L. H. Lin, Optical Holography (Academic, New York, 1971), p. 385.

Marom, E.

Pennington, K. S.

R. J. Collier, K. S. Pennington, “Ghost imaging by holograms formed in the near field,” Appl. Phys. Lett. 8, 44 (1966).
[Crossref]

Restrick, R.

G. W. Stroke, R. Restrick, A. Funkhouser, D. Brumm, “Resolution-retrieving compensation of source effects by correlative reconstruction in high-resolution holography,” Phys. Lett. 18, 274 (1965).
[Crossref]

Stroke, G. W.

G. W. Stroke, R. Restrick, A. Funkhouser, D. Brumm, “Resolution-retrieving compensation of source effects by correlative reconstruction in high-resolution holography,” Phys. Lett. 18, 274 (1965).
[Crossref]

Appl. Opt. (1)

Appl. Phys. Lett. (1)

R. J. Collier, K. S. Pennington, “Ghost imaging by holograms formed in the near field,” Appl. Phys. Lett. 8, 44 (1966).
[Crossref]

Opt. Acta (1)

P. Hariharan, “Statistics of speckle patterns produced by a rough metal surface,” Opt. Acta 24, 979 (1977).
[Crossref]

Phys. Lett. (1)

G. W. Stroke, R. Restrick, A. Funkhouser, D. Brumm, “Resolution-retrieving compensation of source effects by correlative reconstruction in high-resolution holography,” Phys. Lett. 18, 274 (1965).
[Crossref]

Other (1)

R. J. Collier, C. B. Burckhardt, L. H. Lin, Optical Holography (Academic, New York, 1971), p. 385.

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Figures (2)

Fig. 1
Fig. 1

Optical setup.

Fig. 2
Fig. 2

Real-time interference fringes obtained (a) without the reference beam and (b) with the reference beam.

Equations (6)

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t = t B - β I ,
t ( x ) = t B - β O ( x ) + R ( x ) 2 .
A ( x ) = [ O ( x ) + R ( x ) ] t ( x ) ,
A I ( x ) = O ( x ) { t B - β [ O ( x ) 2 + R ( x ) 2 ] } - β O ( x ) R ( x ) 2 .
A I ( x ) 2 = O 0 2 ( x ) ( { t B - β [ O 0 2 ( x ) + R 0 2 ( x ) ] } 2 + β 2 R 0 4 ( x ) - 2 β R 0 2 ( x ) { t B - β [ O 0 2 ( x ) + R 0 2 ( x ) ] } cos Δ ( x ) ) ,
2 β R 0 2 ( x ) { t B - β [ O 0 2 ( x ) + R 0 2 ( x ) ] } ,

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