Abstract

This Letter presents an in-line digital holographic system that can provide full amplitude and phase reconstruction without any reference wave, with a single recorded hologram. This major capability is obtained by using a coherent mixing between several object waves generated by a pure spatial phase modulation. A scaling parameter permits us to reconstruct the phase without any unwrapping. The capability of the method to provide quantitative phase contrast measurement and numerical refocusing is demonstrated through experimental results.

© 2013 Optical Society of America

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References

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2013 (1)

2012 (3)

2011 (2)

2008 (1)

2005 (3)

2001 (1)

P. Picart, R. Mercier, M. Lamare, and J.-M. Breteau, Meas. Sci. Technol. 12, 1311 (2001).
[CrossRef]

2000 (1)

Alfieri, D.

Allano, D.

Bergmann, R. B.

C. Falldorf, C. von Kopylow, and R. B. Bergmann, Proc. SPIE 8413, 84130Q (2012).
[CrossRef]

Bhaduri, B.

Boucheron, R.

Breteau, J.-M.

P. Picart, R. Mercier, M. Lamare, and J.-M. Breteau, Meas. Sci. Technol. 12, 1311 (2001).
[CrossRef]

Cohen, M.

Coppola, G.

Corbin, F.

Cuche, E.

De Nicola, S.

Depeursinge, C.

Desse, J.-M.

Falldorf, C.

C. Falldorf, C. von Kopylow, and R. B. Bergmann, Proc. SPIE 8413, 84130Q (2012).
[CrossRef]

C. Falldorf, J. Opt. Soc. Am. A 28, 1636 (2011).
[CrossRef]

Ferraro, P.

Finizio, A.

Fréchou, D.

Garcia-Sucerquia, J.

Girshovitz, P.

Grilli, S.

Guérineau, N.

Javidi, B.

Kim, M.

Lamare, M.

P. Picart, R. Mercier, M. Lamare, and J.-M. Breteau, Meas. Sci. Technol. 12, 1311 (2001).
[CrossRef]

Lebrun, D.

Lo, C.-M.

Mann, C.

Marquet, P.

Méès, L.

Mercier, R.

P. Picart, R. Mercier, M. Lamare, and J.-M. Breteau, Meas. Sci. Technol. 12, 1311 (2001).
[CrossRef]

Mir, M.

Pham, H.

Picart, P.

J.-M. Desse, P. Picart, and P. Tankam, Opt. Express 16, 5471 (2008).
[CrossRef]

P. Picart, R. Mercier, M. Lamare, and J.-M. Breteau, Meas. Sci. Technol. 12, 1311 (2001).
[CrossRef]

Pierattini, G.

Popescu, G.

Primot, J.

Shaked, N. T.

Striano, V.

Tankam, P.

Velghe, S.

von Kopylow, C.

C. Falldorf, C. von Kopylow, and R. B. Bergmann, Proc. SPIE 8413, 84130Q (2012).
[CrossRef]

Walle, F.

Wattellier, B.

Yu, L.

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Figures (4)

Fig. 1.
Fig. 1.

Basic scheme for the principle of the reference-free digital holographic setup.

Fig. 2.
Fig. 2.

Setup for the in-line holographic recording with a pure spatial phase modulation (MO, microscope objective; L1, tube lens; and SLM, spatial light modulator).

Fig. 3.
Fig. 3.

(a) Estimated phase map φO and (b) comparison between profiles calculated from Ψ (red line) and measured using a Dektak profilometer.

Fig. 4.
Fig. 4.

(a) Out-of-focus image amplitude and (b) phase φO at CCD plane. (c) Profiles of focused and refocused phase contrast image. (d) Noise probability density function.

Equations (4)

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

O(r,kn)=AO(rrn)exp(ikn·r+iφO(rrn)).
H(r)=AO2(r)+n=1n=PAO2(rrn)+2R{n=0P1m=n+1PO(r,kn)O*(r,km)}.
Δφnm(r)=(knkm)·r+φO(rrn)φO(rrm)(knkm)·r+|snm|φO(r)r·enm.
Ψ=λδzpφO=12iπFT1[k=1QβkukD˜kk=1Qβkuk2].

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