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  1. J. P. Huignard, F. Micheron, Appl. Phys. Lett. 29, 591 (1976).
    [CrossRef]
  2. J. P. Huignard, J. P. Herriau, Appl. Opt. 16, 1807 (1977).
    [CrossRef] [PubMed]
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    [CrossRef] [PubMed]
  4. H. Kogelnik, Bell Syst. Tech. J. 48, 2909 (1969).
  5. A. J. Fox, T. M. Bruton, in Proceedings Electrooptic Laser International (United Kingdom, 1976), Vol. 18, p. 131.
  6. G. F. Moore, P. V. Lenzo, E. G. Spencer, A. A. Ballman, J. Appl. Phys. 39, 2361 (1968).
  7. M. P. Petrov, S. I. Stepanov, A. A. Kamshilin, Opt. Commun. 21, 297 (1977).
    [CrossRef]
  8. R. C. Jones, J. Opt. Soc. Am. 38, 671 (1948).
    [CrossRef]
  9. W. J. Tabor, F. S. Chen, J. Appl. Phys. 40, 2760 (1969).
    [CrossRef]
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    [CrossRef] [PubMed]

1977

1976

J. P. Huignard, F. Micheron, Appl. Phys. Lett. 29, 591 (1976).
[CrossRef]

H. Harms, A. Papp, K. Kempter, Appl. Opt. 15, 799 (1976).
[CrossRef] [PubMed]

1969

W. J. Tabor, F. S. Chen, J. Appl. Phys. 40, 2760 (1969).
[CrossRef]

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

1968

G. F. Moore, P. V. Lenzo, E. G. Spencer, A. A. Ballman, J. Appl. Phys. 39, 2361 (1968).

1948

Ballman, A. A.

G. F. Moore, P. V. Lenzo, E. G. Spencer, A. A. Ballman, J. Appl. Phys. 39, 2361 (1968).

Bruton, T. M.

A. J. Fox, T. M. Bruton, in Proceedings Electrooptic Laser International (United Kingdom, 1976), Vol. 18, p. 131.

Chen, F. S.

W. J. Tabor, F. S. Chen, J. Appl. Phys. 40, 2760 (1969).
[CrossRef]

Fox, A. J.

A. J. Fox, T. M. Bruton, in Proceedings Electrooptic Laser International (United Kingdom, 1976), Vol. 18, p. 131.

Harms, H.

Herriau, J. P.

Huignard, J. P.

Jones, R. C.

Kamshilin, A. A.

M. P. Petrov, S. I. Stepanov, A. A. Kamshilin, Opt. Commun. 21, 297 (1977).
[CrossRef]

Kempter, K.

Kogelnik, H.

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

Lenzo, P. V.

G. F. Moore, P. V. Lenzo, E. G. Spencer, A. A. Ballman, J. Appl. Phys. 39, 2361 (1968).

Micheron, F.

J. P. Huignard, F. Micheron, Appl. Phys. Lett. 29, 591 (1976).
[CrossRef]

Moore, G. F.

G. F. Moore, P. V. Lenzo, E. G. Spencer, A. A. Ballman, J. Appl. Phys. 39, 2361 (1968).

Papp, A.

Petrov, M. P.

M. P. Petrov, S. I. Stepanov, A. A. Kamshilin, Opt. Commun. 21, 297 (1977).
[CrossRef]

Spencer, E. G.

G. F. Moore, P. V. Lenzo, E. G. Spencer, A. A. Ballman, J. Appl. Phys. 39, 2361 (1968).

Stepanov, S. I.

M. P. Petrov, S. I. Stepanov, A. A. Kamshilin, Opt. Commun. 21, 297 (1977).
[CrossRef]

Tabor, W. J.

W. J. Tabor, F. S. Chen, J. Appl. Phys. 40, 2760 (1969).
[CrossRef]

Valentin, T.

Appl. Opt.

Appl. Phys. Lett.

J. P. Huignard, F. Micheron, Appl. Phys. Lett. 29, 591 (1976).
[CrossRef]

Bell Syst. Tech. J.

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

J. Appl. Phys.

G. F. Moore, P. V. Lenzo, E. G. Spencer, A. A. Ballman, J. Appl. Phys. 39, 2361 (1968).

W. J. Tabor, F. S. Chen, J. Appl. Phys. 40, 2760 (1969).
[CrossRef]

J. Opt. Soc. Am.

Opt. Commun.

M. P. Petrov, S. I. Stepanov, A. A. Kamshilin, Opt. Commun. 21, 297 (1977).
[CrossRef]

Other

A. J. Fox, T. M. Bruton, in Proceedings Electrooptic Laser International (United Kingdom, 1976), Vol. 18, p. 131.

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Figures (3)

Fig. 1
Fig. 1

(a) Crystallographic orientation of cubic Bi12SiO20 crystals of class 4 ¯ 3 m (crystal size 10 × 10 × 2 mm3, applied voltage 6 kV). (b) Shape of the photoinduced space charge field in thick absorbing BSO crystals at the initial stage of hologram recording (α = 3-cm−1 absorption coefficient and Λ = 1.5-μm fringe spacing).

Fig. 2
Fig. 2

Polarization properties of volume holograms in BSO crystals: (a) Experimentally observed polarization states of diffracted and scattered beams. Permanent readout with retroreflected reference beam. (b) Experimental evidence of scattered noise in the diffracted image. (c) A Polaroid sheet in the image plane provides extinction of scattered beam polarizations (beam ratio = 15, efficiency = 1%, and SNR improvement = +15 dB).

Fig. 3
Fig. 3

The SNR enhancement for nearly on-axis recording configuration: (a) the He–Ne readout beam is elliptically polarized. (b) Reconstructed image of a diffuse object slide. (c) Proper orientation of a polaroid sheet in image plane provides zero order intensity reduction (−15 dB) (crystal size = 10 × 5 × 5 mm3, and Λ = 5 μm).

Equations (3)

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( E x E y ) = ( cos Δ 0 z 0 i sin ψ 0 sin Δ 0 z 0 cos ψ 0 sin Δ 0 z 0 cos ψ 0 sin Δ 0 z 0 cos Δ 0 z 0 + i sin ψ 0 sin Δ 0 z 0 ) ( E x E y ) ,
( ρ 0 2 + θ 0 2 / 4 ) 1 / 2 ,
Δ = ( ρ 2 + θ 2 / 4 ) 1 / 2 , ψ = tan 1 ( θ / 2 ρ ) ,

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