Abstract

Possible applications of polarization holography are demonstratedrecording of pairs of superimposed holograms with one spatial frequency; logical operations on two data arrays recorded simultaneously in the material; double-exposure holographic interferometry.

© 1985 Optical Society of America

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References

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  1. Sh.D. Kakichashvili, “Method for Phase Polarization Recording of Holograms,” Kvantovaya Elektron. Moscow 1, 1435 (1974).
  2. L. Nikolova, T. Todorov, “Diffraction Efficiency and Selectivity of Polarization Holographic Recording,” Opt. Acta 31, 579 (1984).
    [CrossRef]
  3. Sh.D. Kakichashvili, “Polarization Holography,” Vestn. Akad. Nauk SSSR No. 7, 51 (1982).
  4. T. Todorov, L. Nikolova, N. Tomova, “Polarization Holography. 1: A New High-Efficiency Organic Material with Reversible Photoinduced Birefringence,” Appl. Opt. 23, 4309 (1984).
    [CrossRef] [PubMed]
  5. T. Todorov, L. Nikolova, N. Tomova, “Polarization Holography. 2: Polarization Holographic Gratings in Photoanisotropic Materials with and without Intrinsic Birefringence,” Appl. Opt. 23, 4588 (1984).
    [CrossRef] [PubMed]
  6. I. S. Klimenko, V. P. Ryabukho, B. V. Feduleev, N. V. Lokhova, “Some Features of Holographic and Speckle Interferograms Produced by Recording the Object Light Field in the Fourier Plane,” Opt. Spektrosk. 55, 483 (1983)[Opt. Spectrosc. 55, 284 (1983)].

1984

1983

I. S. Klimenko, V. P. Ryabukho, B. V. Feduleev, N. V. Lokhova, “Some Features of Holographic and Speckle Interferograms Produced by Recording the Object Light Field in the Fourier Plane,” Opt. Spektrosk. 55, 483 (1983)[Opt. Spectrosc. 55, 284 (1983)].

1982

Sh.D. Kakichashvili, “Polarization Holography,” Vestn. Akad. Nauk SSSR No. 7, 51 (1982).

1974

Sh.D. Kakichashvili, “Method for Phase Polarization Recording of Holograms,” Kvantovaya Elektron. Moscow 1, 1435 (1974).

Feduleev, B. V.

I. S. Klimenko, V. P. Ryabukho, B. V. Feduleev, N. V. Lokhova, “Some Features of Holographic and Speckle Interferograms Produced by Recording the Object Light Field in the Fourier Plane,” Opt. Spektrosk. 55, 483 (1983)[Opt. Spectrosc. 55, 284 (1983)].

Kakichashvili, Sh.D.

Sh.D. Kakichashvili, “Polarization Holography,” Vestn. Akad. Nauk SSSR No. 7, 51 (1982).

Sh.D. Kakichashvili, “Method for Phase Polarization Recording of Holograms,” Kvantovaya Elektron. Moscow 1, 1435 (1974).

Klimenko, I. S.

I. S. Klimenko, V. P. Ryabukho, B. V. Feduleev, N. V. Lokhova, “Some Features of Holographic and Speckle Interferograms Produced by Recording the Object Light Field in the Fourier Plane,” Opt. Spektrosk. 55, 483 (1983)[Opt. Spectrosc. 55, 284 (1983)].

Lokhova, N. V.

I. S. Klimenko, V. P. Ryabukho, B. V. Feduleev, N. V. Lokhova, “Some Features of Holographic and Speckle Interferograms Produced by Recording the Object Light Field in the Fourier Plane,” Opt. Spektrosk. 55, 483 (1983)[Opt. Spectrosc. 55, 284 (1983)].

Nikolova, L.

Ryabukho, V. P.

I. S. Klimenko, V. P. Ryabukho, B. V. Feduleev, N. V. Lokhova, “Some Features of Holographic and Speckle Interferograms Produced by Recording the Object Light Field in the Fourier Plane,” Opt. Spektrosk. 55, 483 (1983)[Opt. Spectrosc. 55, 284 (1983)].

Todorov, T.

Tomova, N.

Appl. Opt.

Kvantovaya Elektron. Moscow

Sh.D. Kakichashvili, “Method for Phase Polarization Recording of Holograms,” Kvantovaya Elektron. Moscow 1, 1435 (1974).

Opt. Acta

L. Nikolova, T. Todorov, “Diffraction Efficiency and Selectivity of Polarization Holographic Recording,” Opt. Acta 31, 579 (1984).
[CrossRef]

Opt. Spektrosk.

I. S. Klimenko, V. P. Ryabukho, B. V. Feduleev, N. V. Lokhova, “Some Features of Holographic and Speckle Interferograms Produced by Recording the Object Light Field in the Fourier Plane,” Opt. Spektrosk. 55, 483 (1983)[Opt. Spectrosc. 55, 284 (1983)].

Vestn. Akad. Nauk SSSR No. 7

Sh.D. Kakichashvili, “Polarization Holography,” Vestn. Akad. Nauk SSSR No. 7, 51 (1982).

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Figures (9)

Fig. 1
Fig. 1

Setup for polarization holographic recording: Ar—laser; W—Wollaston prism; MO, SP, L—laser beam expander; Pi—input plane; L1—Fourier lens; λ/4 plate; Pf—Fourier plane with medium H for hologram recording; L2—lens for reverse Fourier transformation; A—analyzer; P0—image plane; He–Ne laser; R1,R2—rotators; M—mirror; R,S,R′—object, reference, and reconstructing beams.

Fig. 2
Fig. 2

Reconstructed holograms in superimposed recording: (a) only image I; (b) only image II; (c) two images reconstructed simultaneously.

Fig. 3
Fig. 3

Same as Fig. 2 for another pair of objects.

Fig. 4
Fig. 4

Reconstructed holograms on which two circles with different diameters are superimposed: (a) bigger circle; (b) smaller circle; (c) difference between the two circles.

Fig. 5
Fig. 5

Setup for recording reflective objects. Designations are as in Fig. 1. The position of the reflective object is O.

Fig. 6
Fig. 6

Interferogram from reconstruction of a double-exposure hologram.

Fig. 7
Fig. 7

Reconstructed image from a double-exposure polarization interferogram without analyzer A.

Fig. 8
Fig. 8

Polarization interferograms of transparent object visualizing the phase shifts between the exposures. Rotation of R2 enhances interference contrast.

Fig. 9
Fig. 9

Rotation of analyzer A results in continuous shift of interference pattern (a),(b),(c). This ensures better visualization of any point on the interferogram (d),(e).

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