Abstract

We propose and experimentally demonstrate a novel dot-array recording method in which rainbow holograms are used for the purpose of making hard copies of three-dimensional image data stored in computers.

© 1996 Optical Society of America

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References

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    [CrossRef]
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1993 (1)

1992 (2)

1991 (1)

L. Z. Cai, Opt. Commun. 81, 6 (1991).
[CrossRef]

1990 (1)

C. Guo, Acta Opt. Sinica 10, 991 (1990).

1989 (1)

1987 (1)

N. Ohyaha, Y. Minami, A. Watanabe, J. Tsujiuchi, T. Honda, Opt. Commun. 61, 96 (1987).
[CrossRef]

1984 (2)

1978 (1)

1969 (1)

S. A. Benton, J. Opt. Soc. Am. 59, 1545 (1969).

Benton, S. A.

S. A. Benton, J. Opt. Soc. Am. 59, 1545 (1969).

Bryngdahl, O.

Cai, L. Z.

Chen, H.

Guo, C.

L. Z. Cai, C. Guo, Opt. Lett. 18, 69 (1993).
[CrossRef] [PubMed]

C. Guo, Acta Opt. Sinica 10, 991 (1990).

Haneishi, H.

Honda, T.

Inoue, S.

Leseberg, D.

Minami, Y.

N. Ohyaha, Y. Minami, A. Watanabe, J. Tsujiuchi, T. Honda, Opt. Commun. 61, 96 (1987).
[CrossRef]

Ohyaha, N.

N. Ohyaha, Y. Minami, A. Watanabe, J. Tsujiuchi, T. Honda, Opt. Commun. 61, 96 (1987).
[CrossRef]

Ohyama, N.

Tsujiuchi, J.

N. Ohyama, S. Inoue, H. Haneishi, J. Tsujiuchi, T. Honda, Appl. Opt. 28, 5338 (1989).
[CrossRef] [PubMed]

N. Ohyaha, Y. Minami, A. Watanabe, J. Tsujiuchi, T. Honda, Opt. Commun. 61, 96 (1987).
[CrossRef]

Watanabe, A.

N. Ohyaha, Y. Minami, A. Watanabe, J. Tsujiuchi, T. Honda, Opt. Commun. 61, 96 (1987).
[CrossRef]

Yamaguchi, M.

Yu, F. T. S.

Zhang, Y. W.

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Figures (5)

Fig.1
Fig.1

Recording principle of the DARH.

Fig.2
Fig.2

Geometric perspective of a 3D object O, projected onto the slit LC as a dot, D, on hologram plate H.

Fig.3
Fig.3

Reconstruction of the DARH.

Fig. 4
Fig. 4

Experimental setup of the DARH: M1–M3, mirrors; BS, beam splitter; PC, personal computer.

Fig. 5
Fig. 5

Experimental results showing two reconstructed images viewed from (a) the left and (b) the right direction.

Equations (4)

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χ i = l Z n ( χ n χ m ) + χ m ,
y j = l Z n y n .
cos ( Δ α i ) = χ i ( χ i 2 + y j 2 + l 2 ) 1 / 2 ,
cos ( β 0 + Δ β j ) cos β 0 = y j ( χ i 2 + y j 2 + l 2 ) 1 / 2 .

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