Abstract

We propose and demonstrate a nonvolatile holographic recording system for storing two-dimensional images. The readout light in this system is not absorbed by the holographic medium, and the data are preformatted or postformatted so that lines from different holograms are interleaved to satisfy the Bragg-matching condition.

© 1994 Optical Society of America

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References

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1993 (3)

1992 (3)

1991 (2)

1990 (1)

1989 (1)

1988 (1)

1986 (1)

1975 (1)

D. L. Staebler, W. J. Burke, W. Phillips, J. J. Amodei, Appl. Phys. Lett. 26, 182 (1975).
[CrossRef]

1972 (1)

F. Micheron, G. Bismuth, Appl. Phys. Lett. 20, 79 (1972).
[CrossRef]

Amodei, J. J.

D. L. Staebler, W. J. Burke, W. Phillips, J. J. Amodei, Appl. Phys. Lett. 26, 182 (1975).
[CrossRef]

An, X.

D. Psaltis, H.-Y. S. Li, X. An, Proc. Soc. Photo-Opt. Instrum. Eng. 2026, B43 (1993).

Bismuth, G.

F. Micheron, G. Bismuth, Appl. Phys. Lett. 20, 79 (1972).
[CrossRef]

Boj, S.

Brady, D.

Burke, W. J.

D. L. Staebler, W. J. Burke, W. Phillips, J. J. Amodei, Appl. Phys. Lett. 26, 182 (1975).
[CrossRef]

Delboulbe, A.

Fainman, Y.

Ford, J. E.

Goodman, J.

Herriau, J. P.

Hesselink, L.

Hsu, K.

Huignard, J. P.

Külich, H.-C.

Lee, S.

Li, H.-Y. S.

D. Psaltis, H.-Y. S. Li, X. An, Proc. Soc. Photo-Opt. Instrum. Eng. 2026, B43 (1993).

McRuer, R.

Micheron, F.

F. Micheron, G. Bismuth, Appl. Phys. Lett. 20, 79 (1972).
[CrossRef]

Mok, F. H.

Neurgaonkar, R. R.

Orlov, S.

Pauliat, G.

Phillips, W.

D. L. Staebler, W. J. Burke, W. Phillips, J. J. Amodei, Appl. Phys. Lett. 26, 182 (1975).
[CrossRef]

Psaltis, D.

Qiao, Y.

Redfield, S.

Roosen, G.

Sasaki, H.

Staebler, D. L.

D. L. Staebler, W. J. Burke, W. Phillips, J. J. Amodei, Appl. Phys. Lett. 26, 182 (1975).
[CrossRef]

Taketomi, Y.

Wilde, J.

Yong, Q.

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Figures (4)

Fig. 1
Fig. 1

Setup for recording and retrieving two-dimensional images by use of two wavelengths. L2, imaging lens.

Fig. 2
Fig. 2

k-space diagram of the Bragg-matching condition in the two-wavelength system.

Fig. 3
Fig. 3

(a) k-space cross-section diagram and (b) interleaving scheme for multiple holograms using the two-wavelength system. The holograms #1, #2, and #3 are recorded at different reference beam angles. On reconstruction with λ2, only one line from each hologram appears.

Fig. 4
Fig. 4

Experimental results: (a) reconstructed hologram of the first image using the λ1 plane-wave reference beam, (b) reconstructed hologram of the second image using the λ1 plane-wave reference beam, (c) reconstructed hologram using λ2, consisting of two lines from each of the two images. The first line (B) comes from the second image, and the second line (A) comes from the first image.

Equations (3)

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L = 2 λ 1 F Δ x w 1 tan ( θ 2 θ 1 ) ,
sin θ 1 λ 1 = sin θ 2 λ 2 .
Δ θ 1 R = sin ( θ 2 θ 1 ) sin ( θ 2 + θ 1 ) Δ x l n F ,

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