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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    [Crossref]
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    [Crossref]
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    [Crossref]
  15. N. Demoli, J. Meštrović, and I. Sović, “Subtraction digital holography,” Appl. Opt. 42, 798–804 (2003).
    [Crossref] [PubMed]
  16. 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]
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    [Crossref]
  18. T. H. Jeong, H. I. Bjelkhagen, and L. M. Spoto, “Holographic interferometry with multiple wavelengths,” Appl. Opt. 36, 3686–3688 (1997).
    [Crossref] [PubMed]
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    [Crossref]
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    [Crossref]
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    [Crossref]

2003 (1)

2002 (6)

2001 (3)

2000 (3)

A. Stadelmaier and J. H. Massing, “Compensation of lens aberrations in digital holography,” Opt. Lett. 25, 1630–1632 (2000).
[Crossref]

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

S. Murata and N. Yasuda, “Potential of digital holography in particle measurement,” Opt. Las. Technol. 32, 567–574 (2000).
[Crossref]

1999 (3)

Y. Takaki and H. Ohzu, “Fast numerical reconstruction technique for high-resolution hybrid holographic microscopy,” Appl. Opt. 38, 2204–2211 (1999).
[Crossref]

G. Pedrini, P. Fröning, H. Tiziani, and F. Santoyo, “Shape mesurement of microscopic structures using digital holograms,” Opt. Commun. 164, 257–268 (1999).
[Crossref]

D. Vukicevic, M. Torzynski, and I. El-Haffidi, “Color holographic interferometry,” Proc. SPIE 3783, 294–301 (1999).
[Crossref]

1997 (4)

T. M. Kreis and W. P. O. Jüptner, “Suppression of the dc term in digital holography,” Opt. Eng. 36, 2357–2360 (1997).
[Crossref]

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]

J. M. Desse, “Three-color differential interferometry,” Appl. Opt. 36, 7150–7156 (1997).
[Crossref]

T. H. Jeong, H. I. Bjelkhagen, and L. M. Spoto, “Holographic interferometry with multiple wavelengths,” Appl. Opt. 36, 3686–3688 (1997).
[Crossref] [PubMed]

Aggarwal, A. K.

Albe, F.

J. M. Desse, F. Albe, and J.-L. Tribillon,“Real-time color holographic interferometry,” Appl. Opt. 41, 5325–5333 (2002).
[Crossref]

Baumbach, T.

Benoit, M. R.

Binet, R.

Bjelkhagen, H. I.

Centurion, M.

Colineau, J.

De Nicola, S.

Demoli, N.

Desse, J. M.

J. M. Desse, F. Albe, and J.-L. Tribillon,“Real-time color holographic interferometry,” Appl. Opt. 41, 5325–5333 (2002).
[Crossref]

J. M. Desse, “Three-color differential interferometry,” Appl. Opt. 36, 7150–7156 (1997).
[Crossref]

Dezhong, W.

W. Dezhong and Z. Tiange, “The measurement of 3-D asymmetric temperature field by using real time laser interferometric tomography,” Optics and Lasers in Engineering 36, 289–297 (2001).
[Crossref]

El-Haffidi, I.

D. Vukicevic, M. Torzynski, and I. El-Haffidi, “Color holographic interferometry,” Proc. SPIE 3783, 294–301 (1999).
[Crossref]

Ferraro, P.

Finizio, A.

Fröning, P.

G. Pedrini, P. Fröning, H. Tiziani, and F. Santoyo, “Shape mesurement of microscopic structures using digital holograms,” Opt. Commun. 164, 257–268 (1999).
[Crossref]

Grilli, S.

Harthong, J.

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]

Hayes, J.

J. Hayes, “Dynamic interferometry handles vibration,” Laser Focus World, 109–113 (2002).

Hong, J.

Jeong, T. H.

Jüptner, W.

Jüptner, W. P. O.

T. M. Kreis and W. P. O. Jüptner, “Suppression of the dc term in digital holography,” Opt. Eng. 36, 2357–2360 (1997).
[Crossref]

Kato, J.

King, B.

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

Klaus, D. M.

Kreis, T.

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

Kreis, T. M.

T. M. Kreis and W. P. O. Jüptner, “Suppression of the dc term in digital holography,” Opt. Eng. 36, 2357–2360 (1997).
[Crossref]

Lai, S.

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

Lehureau, J.-C.

Liu, Z.

Massing, J. H.

Matsumura, T.

Meštrovic, J.

Meucci, R.

Murata, S.

S. Murata and N. Yasuda, “Potential of digital holography in particle measurement,” Opt. Las. Technol. 32, 567–574 (2000).
[Crossref]

Neifield, M. A.

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

Ohzu, H.

Osten, W.

Owen, R. B.

Panotopoulos, G.

Pedrini, G.

S. Schedin, G. Pedrini, H. J. Tiziani, and A. K. Aggarwal, “Comparative study of various endoscopes for pulsed digital holographic interferometry,” Appl. Opt. 40, 2692–2697 (2001).
[Crossref]

G. Pedrini, P. Fröning, H. Tiziani, and F. Santoyo, “Shape mesurement of microscopic structures using digital holograms,” Opt. Commun. 164, 257–268 (1999).
[Crossref]

Pierattini, G.

Psaltis, D.

Sadi, J.

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]

Santoyo, F.

G. Pedrini, P. Fröning, H. Tiziani, and F. Santoyo, “Shape mesurement of microscopic structures using digital holograms,” Opt. Commun. 164, 257–268 (1999).
[Crossref]

Schedin, S.

Sovic, I.

Spoto, L. M.

Stadelmaier, A.

Takaki, Y.

Tiange, Z.

W. Dezhong and Z. Tiange, “The measurement of 3-D asymmetric temperature field by using real time laser interferometric tomography,” Optics and Lasers in Engineering 36, 289–297 (2001).
[Crossref]

Tiziani, H.

G. Pedrini, P. Fröning, H. Tiziani, and F. Santoyo, “Shape mesurement of microscopic structures using digital holograms,” Opt. Commun. 164, 257–268 (1999).
[Crossref]

Tiziani, H. J.

Torzynski, M.

D. Vukicevic, M. Torzynski, and I. El-Haffidi, “Color holographic interferometry,” Proc. SPIE 3783, 294–301 (1999).
[Crossref]

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]

Tribillon, J.-L.

J. M. Desse, F. Albe, and J.-L. Tribillon,“Real-time color holographic interferometry,” Appl. Opt. 41, 5325–5333 (2002).
[Crossref]

Vukicevic, D.

D. Vukicevic, M. Torzynski, and I. El-Haffidi, “Color holographic interferometry,” Proc. SPIE 3783, 294–301 (1999).
[Crossref]

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]

Yamaguchi, I.

Yasuda, N.

S. Murata and N. Yasuda, “Potential of digital holography in particle measurement,” Opt. Las. Technol. 32, 567–574 (2000).
[Crossref]

Zozulya, A. A.

Appl. Opt. (8)

J. Opt. Soc. Am A (1)

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]

Opt. Commun. (2)

S. Lai, B. King, and 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, and F. Santoyo, “Shape mesurement of microscopic structures using digital holograms,” Opt. Commun. 164, 257–268 (1999).
[Crossref]

Opt. Eng. (1)

T. M. Kreis and W. P. O. Jüptner, “Suppression of the dc term in digital holography,” Opt. Eng. 36, 2357–2360 (1997).
[Crossref]

Opt. Express (1)

Opt. Las. Technol. (1)

S. Murata and N. Yasuda, “Potential of digital holography in particle measurement,” Opt. Las. Technol. 32, 567–574 (2000).
[Crossref]

Opt. Lett. (4)

Optics and Lasers in Engineering (1)

W. Dezhong and Z. Tiange, “The measurement of 3-D asymmetric temperature field by using real time laser interferometric tomography,” Optics and Lasers in Engineering 36, 289–297 (2001).
[Crossref]

Proc. SPIE (1)

D. Vukicevic, M. Torzynski, and I. El-Haffidi, “Color holographic interferometry,” Proc. SPIE 3783, 294–301 (1999).
[Crossref]

Other (2)

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

J. Hayes, “Dynamic interferometry handles vibration,” Laser Focus World, 109–113 (2002).

Supplementary Material (1)

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Figures (6)

Fig. 1.
Fig. 1.

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

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Fig. 2.
Fig. 2.

Phase object used in experiments.

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Fig. 3.
Fig. 3.

Object reconstruction obtained from the three monochromatic digital holograms.

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Fig. 4.
Fig. 4.

First four color digital holographic interferograms.

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Fig. 5.
Fig. 5.

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

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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.

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Equations (14)

Equations on this page are rendered with MathJax. Learn more.

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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