Abstract

We propose synthetic aperture integral imaging, in which an effectively enlarged aperture (or field of view) is obtained by movement of small integral imaging system. This system substantially increases the field of view and the viewing resolution. The feasibility of our approach is experimentally demonstrated. To the best of our knowledge, this is the first time the synthetic aperture technique has been applied to three-dimensional integral imaging.

© 2002 Optical Society of America

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References

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2002 (1)

2001 (3)

1998 (1)

1997 (1)

1968 (1)

1908 (1)

G. Lippmann, C. R. Acad. Sci. 146, 446 (1908).

Arai, J.

Arimoto, H.

Burckhardt, C. B.

Erdmann, L.

Gabriel, K. J.

Goodman, J.

J. Goodman, Introduction to Fourier Optics (McGraw-Hill, New York, 1996).

Hoshino, H.

Isono, H.

Jang, J.-S.

Javidi, B.

Jung, S.

Lee, B.

Lippmann, G.

G. Lippmann, C. R. Acad. Sci. 146, 446 (1908).

Min, S.-W.

Okano, F.

Park, J.-H.

Yuma, I.

Yuyama, I.

Appl. Opt. (3)

C. R. Acad. Sci. (1)

G. Lippmann, C. R. Acad. Sci. 146, 446 (1908).

J. Opt. Soc. Am. (1)

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

Opt. Lett. (2)

Other (2)

B. Javidi and F. Okano, eds., Three Dimensional Television, Video, and Display Technology (Springer-Verlag, Berlin, 2002).

J. Goodman, Introduction to Fourier Optics (McGraw-Hill, New York, 1996).

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Figures (6)

Fig. 1
Fig. 1

3D image recording and display.

Fig. 2
Fig. 2

Concept of SAII. Abbreviations defined in text.

Fig. 3
Fig. 3

3D object used in the experiments.

Fig. 4
Fig. 4

Experimental setup: II system with an optically addressed SLM (LCLV).

Fig. 5
Fig. 5

Reconstructed images when the II system is stationary. Only part of the toy car can be reconstructed at a time, because the aperture of the II system is limited.

Fig. 6
Fig. 6

Experimental result for SAII

Equations (1)

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V>maxpScos θ+Vmax,x,pSsin θ+Vmax,y,

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