Abstract

A color digital holographic interferometry movie was produced by applying the subtraction digital holography method in a quasi-Fourier off-axis experimental setup. The movie was numerically recorded and replayed from three sets of digital holograms obtained with three different laser lines (476 nm, 532 nm, and 647 nm). The movie shows convective flows induced by thermal dissipation in a tank filled with oil.

© 2003 Optical Society of America

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References

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Appl. Opt.

J. Opt. Soc. Am A

J. Harthong, J. Sadi, M. Torzynski, and D. Vukicevic, "Speckle phase averagingin high resolution color holography," J. Opt. Soc. Am A 14, 405-410 (1997).
[CrossRef]

Laser Focus World

J. Hayes, "Dynamic interferometry handles vibration," Laser Focus World, 109-113 (2002)

Opt. Commun.

S. Lai, B. King, M. A. Neifield, "Wave front reconstruction by means of phase-shifting digital in-line holography," Opt. Commun. 173, 155-160 (2000).
[CrossRef]

G. Pedrini, P. Fröning, H. Tiziani, F. Santoyo, "Shape mesurement of microscopic structures using digital holograms," Opt. Commun. 164, 257-268 (1999).
[CrossRef]

Opt. Eng.

T. M. Kreis, W. P. O. Jüptner, "Suppression of the dc term in digital holography," Opt. Eng. 36, 2357-2360 (1997).
[CrossRef]

Opt. Express

Opt. Las. Technol.

S. Murata, N. Yasuda, "Potential of digital holography in particle measurement," Opt. Las. Technol. 32, 567-574 (2000).
[CrossRef]

Opt. Lasers Eng.

W. Dezhong, Z. Tiange, "The measurement of 3-D asymmetric temperature field by using real time laser interferometric tomography," Opt. Lasers Eng. 36, 289-297 (2001).
[CrossRef]

Opt. Lett.

Proc. SPIE

D. Vukicevic, M. Torzynski, I. El-Haffidi, "Color holographic interferometry," Proc. SPIE 3783, 294-301 (1999).
[CrossRef]

Other

T. Kreis, Holographic Interferometry, Principles and Methods (Academie Verlag, Berlin, 1996).

Supplementary Material (1)

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Figures (6)

Fig. 1.
Fig. 1.

Experimental setup for recording quasi-Fourier off-axis digital holograms.

Fig. 2.
Fig. 2.

Phase object used in experiments.

Fig. 3.
Fig. 3.

Object reconstruction obtained from the three monochromatic digital holograms.

Fig. 4.
Fig. 4.

First four color digital holographic interferograms.

Fig. 5.
Fig. 5.

Red component of the color interferograms shown in Fig. 4.

Fig. 6.
Fig. 6.

(1.76 MB) Color movie of convective flows induced by thermal dissipation, composed from the sequence of digital holographic interferometry images.

Equations (14)

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u x 1 y 1 = R 0 δ x 1 x 0 y 1 y 0 + S 0 exp [ i 2 π λ n x 1 y 1 z d z ] ,
u x 2 y 2 = R 0 C 0 exp { i ψ x 2 y 2 } + s x 2 y 2 ,
s x 2 y 2 = α · S 0 ,
I ( x 2 , y 2 ) = ( R 0 λd ) 2 + s ( x 2 , y 2 ) 2
+ R 0 λd s ( x 2 , y 2 ) exp [ i ψ ( x 2 , y 2 ) ] + R 0 λd s * ( x 2 , y 2 ) exp [ i ψ ( x 2 , y 2 ) ] ,
I ( x 2 , y 2 , t n ) = ( R 0 λd ) 2 + s ( x 2 , y 2 , t n ) 2
+ R 0 λd s ( x 2 , y 2 , t n ) exp [ i ψ ( x 2 , y 2 ) ] + R 0 λd s * ( x 2 , y 2 , t n ) exp [ i ψ ( x 2 , y 2 ) ]
Δ I ( x 2 , y 2 , t n ) = I ( x 2 , y 2 , t 0 ) I ( x 2 , y 2 , t n )
[ s ( x 2 , y 2 , t 0 ) s ( x 2 , y 2 , t n ) ] exp [ i ψ ( x 2 , y 2 ) ] + C C
s ( x 2 , y 2 , t n ) exp [ i φ ( x 2 , y 2 , t 0 ) + φ ( x 2 , y 2 , t n ) 2 ] × sin [ Δ φ ( x 2 , y 2 , t n ) 2 ]
× exp [ i π λd ( x 2 2 + y 2 2 ) ] × exp [ i 2 π λd ( x 2 x 0 + y 2 y 0 ) ] + C C ,
Δ φ ( x 2 , y 2 , t n ) = 2 π λ Δ n ( x 2 , y 2 , z , t n ) d z ,
Δ n ( x 2 , y 2 , z , t n ) = n ( x 2 , y 2 , z , t 0 ) n ( x 2 , y 2 , z , t n )
Δ n ( x 2 , y 2 , z , t n ) d z = m λ ( x 2 , y 2 , t n ) λ , m λ = 0 , 1 , 2 ,

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