Abstract

Multiwavelength recording and reconstruction of a three-dimensional object are realized by use of phase-shifting digital holography. Red, green, and blue lines emitted from a white-light He–Cd laser are used for one-step recording of the complex amplitude of the object with a color CCD camera, in which a phase shift is introduced with an achromatic phase shifter based on the geometric phase. Three color images are reconstructed and successfully combined in a computer by use of Fresnel transformation based on a convolution.

© 2002 Optical Society of America

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2002 (1)

2001 (1)

2000 (1)

1998 (1)

1997 (3)

1996 (1)

1994 (2)

U. Schnars and W. Jüptner, Appl. Opt. 33, 179 (1994).
[CrossRef] [PubMed]

P. Hariharan and P. E. Ciddor, Opt. Commun. 110, 13 (1994).
[CrossRef]

1991 (1)

T. Kubota, J. Opt. 22, 267 (1991).
[CrossRef]

1975 (1)

Y. Aoki, T. Iwasaki, Y. Suzuki, and S. Ishizuka, Electron. Commun. Jpn. 58, 136 (1975).

1974 (1)

Y. Aoki and S. Ishizuka, Electron. Commun. Jpn. 57, 90 (1974).

1967 (1)

J. W. Goodman and R. W. Lawrence, Appl. Phys. Lett. 11, 77 (1967).
[CrossRef]

Aoki, Y.

Y. Aoki, T. Iwasaki, Y. Suzuki, and S. Ishizuka, Electron. Commun. Jpn. 58, 136 (1975).

Y. Aoki and S. Ishizuka, Electron. Commun. Jpn. 57, 90 (1974).

Ciddor, P. E.

P. Hariharan and P. E. Ciddor, Opt. Commun. 110, 13 (1994).
[CrossRef]

Dorsch, R. G.

Garcia, J.

Goodman, J. W.

J. W. Goodman and R. W. Lawrence, Appl. Phys. Lett. 11, 77 (1967).
[CrossRef]

Hariharan, P.

P. Hariharan and P. E. Ciddor, Opt. Commun. 110, 13 (1994).
[CrossRef]

Ishizuka, S.

Y. Aoki, T. Iwasaki, Y. Suzuki, and S. Ishizuka, Electron. Commun. Jpn. 58, 136 (1975).

Y. Aoki and S. Ishizuka, Electron. Commun. Jpn. 57, 90 (1974).

Iwasaki, T.

Y. Aoki, T. Iwasaki, Y. Suzuki, and S. Ishizuka, Electron. Commun. Jpn. 58, 136 (1975).

Javidi, B.

Jüptner, W.

Kato, J.

Kubota, T.

T. Kubota, J. Opt. 22, 267 (1991).
[CrossRef]

Kuwashima, S.

Lawrence, R. W.

J. W. Goodman and R. W. Lawrence, Appl. Phys. Lett. 11, 77 (1967).
[CrossRef]

Mas, D.

Matsumura, T.

Mizuno, J.

Nakamura, T.

Ohta, S.

Pedrini, G.

G. Pedrini and H. J. Tiziani, Opt. Laser Technol. 29, 249 (1997).
[CrossRef]

Schnars, U.

Suzuki, Y.

Y. Aoki, T. Iwasaki, Y. Suzuki, and S. Ishizuka, Electron. Commun. Jpn. 58, 136 (1975).

Tajahuerce, E.

Tiziani, H. J.

G. Pedrini and H. J. Tiziani, Opt. Laser Technol. 29, 249 (1997).
[CrossRef]

Yamaguchi, I.

Zhang, T.

Appl. Opt. (5)

Appl. Phys. Lett. (1)

J. W. Goodman and R. W. Lawrence, Appl. Phys. Lett. 11, 77 (1967).
[CrossRef]

Electron. Commun. Jpn. (2)

Y. Aoki, T. Iwasaki, Y. Suzuki, and S. Ishizuka, Electron. Commun. Jpn. 58, 136 (1975).

Y. Aoki and S. Ishizuka, Electron. Commun. Jpn. 57, 90 (1974).

J. Opt. (1)

T. Kubota, J. Opt. 22, 267 (1991).
[CrossRef]

Opt. Commun. (1)

P. Hariharan and P. E. Ciddor, Opt. Commun. 110, 13 (1994).
[CrossRef]

Opt. Laser Technol. (1)

G. Pedrini and H. J. Tiziani, Opt. Laser Technol. 29, 249 (1997).
[CrossRef]

Opt. Lett. (3)

Other (1)

http://www.fftw.org .

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Figures (5)

Fig. 1
Fig. 1

Optical configuration for multicolor phase-shifting digital holography with an achromatic phase shifter. M’s, mirrors. Other abbreviations defined in text.

Fig. 2
Fig. 2

Dependences of the amount of phase shift and the contrast variations on the rotation angle of HWP1 in the achromatic phase shifter for three wavelengths: (a) He–Ne laser λ=632.8 nm, (b) Ar+ laser λ=514.5 nm, and (c) Ar+ laser λ=457.9 nm.

Fig. 3
Fig. 3

Reconstruction results for the green wavelength (a) before and (b) after noise reduction in the reconstruction process.

Fig. 4
Fig. 4

Focused images reconstructed at Z=380 mm for each wavelength from captured holograms with a He–Cd white-light laser: (a) red λ=636.0 nm, (b) green λ=537.8 nm, (c) blue λ=441.6 nm. The object is an embossed relief image of Peko-chan (©Fujiya).

Fig. 5
Fig. 5

Unification results of reconstructed RGB images: (a) ordinary image taken by the color CCD camera with an imaging lens. Unified images reconstructed at (b) Z=280 mm, (c) Z=380 mm, and (d) Z=480 mm are also shown.

Equations (2)

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UHx,y,λ=IHx,y,λ;0-IHx,y,λ;π+iIHx,y,λ;π2-IHx,y,λ;3π2.
URX,Y,Z,λ=expi2πλx2+y22ZUHx,y,λ.

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