Abstract

We have developed a modified version of a scanning holography microscope in which the Fresnel Zone Plates (FZP) are created by a homodyne rather than a heterodyne interferometer. Therefore, during the scanning the projected pattern on the specimen is frozen rather than varied as previously. In each scanning period the system produces an on-axis Fresnel hologram. The twin image problem is solved by a linear combination of at least three holograms taken with three FZPs with different phase values.

© 2006 Optical Society of America

Full Article  |  PDF Article

References

  • View by:
  • |
  • |
  • |

  1. I. Yamaguchi and T. Zhang, "Phase-shifting digital holography," Opt. Lett. 22, 1268-1269 (1997).
    [CrossRef] [PubMed]
  2. B. W. Schilling, T.-C. Poon, G. Indebetouw, B. Storrie, K. Shinoda, Y. Suzuki, and M. H. Wu, "Three-dimensional holographic fluorescence microscopy," Opt. Lett. 22, 1506-1508 (1997).
    [CrossRef]
  3. G. Indebetouw, A. El Maghnouji, and R. Foster, "Scanning holographic microscopy with transverse resolution exceeding the Rayleigh limit and extended depth of focus," J. Opt. Soc. Am. A 22, 892-898 (2005).
    [CrossRef]
  4. G. Indebetouw, P. Klysubun, T. Kim, and T.-C. Poon, "Imaging properties of scanning holographic microscopy," J. Opt. Soc. Am. A 17,380-390(2000).
    [CrossRef]
  5. J. W. Goodman, Introduction to Fourier Optics, 2nd ed. (McGraw-Hill, New York, 1996), 126-165.

2005

2000

1997

El Maghnouji, A.

Foster, R.

Indebetouw, G.

Kim, T.

Klysubun, P.

Poon, T.-C.

Schilling, B. W.

Shinoda, K.

Storrie, B.

Suzuki, Y.

Wu, M. H.

Yamaguchi, I.

Zhang, T.

Supplementary Material (1)

» Media 1: AVI (4480 KB)     

Cited By

OSA participates in CrossRef's Cited-By Linking service. Citing articles from OSA journals and other participating publishers are listed here.

Alert me when this article is cited.


Figures (4)

Fig. 1.
Fig. 1.

Optical setup: EOPM, electro-optic phase modulator introducing a phase difference between the two beams; BS, beam splitter; PI, piezo XY stage, OBJ, objective; PM, photomultiplier tube detector; LPF, lowpass filter; PC, personal computer.

Fig. 2.
Fig. 2.

Three recorded holograms with phase difference between the two interferometers arms of (a) 0 (b) π/2 and (c) π.

Fig. 3.
Fig. 3.

(a) The magnitude and (b) The phase of the final hologram. [Media 1]

Fig. 4.
Fig. 4.

Movie of the image reconstruction along the light propagation axis.

Equations (8)

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

F ( x , y , z ) = Ap ( x , y ) { 2 + exp [ i π λ ( γ + z ) ( x 2 + y 2 ) + i θ ] + exp [ i π λ ( γ + z ) ( x 2 + y 2 ) i θ ] } ,
O ( x , y ; γ ) = S ( x , y , z ) * F ( x , y , z ) = 2 A S ( x , y , z ) * p ( x , y ) dz
+ A S ( x , y , z ) p ( x x , y y ) exp { i π [ ( x x ) 2 + ( y y ) 2 ] λ ( γ + z ) + i θ } dx dy dz
+ A S ( x , y , z ) p ( x x , y y ) exp { i π [ ( x x ) 2 + ( y y ) 2 ] λ ( γ + z ) i θ } dx dy dz ,
O F ( x , y ; γ ) = O 1 ( x , y ; γ ) [ exp ( ± i θ 3 ) exp ( ± i θ 2 ) ] + O 2 ( x , y ; γ ) [ exp ( ± i θ 1 ) exp ( ± i θ 3 ) ]
+ O 3 ( x , y ; γ ) [ exp ( ± i θ 2 ) exp ( ± i θ 1 ) ] ,
O F ( x , y ; γ ) = S ( x , y , z ) * p ( x , y ) exp [ i π λ ( γ + z ) ( x 2 + y 2 ) ] dz .
S ( x , y , z ) = O F ( x , y ; γ ) * exp [ i π 2 λ z ( x 2 + y 2 ) ] .

Metrics