Abstract

We demonstrate recording and reconstruction of multiple-computer-generated wavelength-multiplexed volume holograms in a holographic storage medium. The holograms display high selectivity, and their reconstruction process results in a convenient conversion of wavelength into angular multiplexing.

© 1993 Optical Society of America

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References

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  1. J. Rosen, L. Shiv, J. Stein, J. Shamir, J. Opt. Soc. Am. A 9, 1159 (1992), and references therein.
    [Crossref]
  2. L. Pugliese, G. M. Morris, Opt. Lett. 15, 338 (1990).
    [Crossref] [PubMed]
  3. H. Kogelnick, Bell Syst. Tech. J. 48, 2909 (1969).
  4. J. P. Allebach, D. W. Sweeny, Proc. Soc. Photo-Opt. Instrum. Eng. 884, 2 (1988).
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    [Crossref] [PubMed]

1992 (1)

1990 (1)

1989 (1)

1988 (1)

J. P. Allebach, D. W. Sweeny, Proc. Soc. Photo-Opt. Instrum. Eng. 884, 2 (1988).

1969 (1)

H. Kogelnick, Bell Syst. Tech. J. 48, 2909 (1969).

Appl. Opt. (1)

Bell Syst. Tech. J. (1)

H. Kogelnick, Bell Syst. Tech. J. 48, 2909 (1969).

J. Opt. Soc. Am. A (1)

Opt. Lett. (1)

Proc. Soc. Photo-Opt. Instrum. Eng. (1)

J. P. Allebach, D. W. Sweeny, Proc. Soc. Photo-Opt. Instrum. Eng. 884, 2 (1988).

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Figures (2)

Fig. 1
Fig. 1

Experimental setup for computer generation and recording of volume holograms. BS, beam splitter.

Fig. 2
Fig. 2

a, Detailed drawing demonstrating the reconstruction and its angular dependence on the tilted wavelength-multiplexed volume holograms. b, Binary CGH. c, Direct reconstruction from the SLM with an He–Ne laser. d, Reconstructions from the volume holographic medium with the He–Ne and Ar lasers simultaneously. The right image (T) is red, while the left image (S) is green.

Equations (1)

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Λ 1 / Λ 0 = [ λ 0 n ( λ 1 ) + λ 1 n ( λ 0 ) ] / 2 λ 0 n ( λ 0 ) ,

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