Hologram reconstruction corrected for measurements through layers with different refractive indices in digital in-line holographic microscopy
Digital in-line holographic microscopy (DIHM) using point sources has been shown to be a versatile technique, especially for three-dimensional tracking of particles or microorganisms. However, the spherical source wave is altered when measurements are performed through layers with different refracti...
Gespeichert in:
| Hauptverfasser: | , , , |
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| Dokumenttyp: | Article (Journal) |
| Sprache: | Englisch |
| Veröffentlicht: |
30 May 2012
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| In: |
Applied optics
Year: 2012, Jahrgang: 51, Heft: 16, Pages: 3416-3423 |
| ISSN: | 2155-3165 |
| DOI: | 10.1364/AO.51.003416 |
| Online-Zugang: | Verlag, Volltext: http://dx.doi.org/10.1364/AO.51.003416 Verlag, Volltext: https://www.osapublishing.org/ao/abstract.cfm?uri=ao-51-16-3416 
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| Verfasserangaben: | Gonzalo H. Sendra, Sebastian Weisse, Stojan Maleschlijski, and Axel Rosenhahn |
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| 245 | 1 | 0 | |a Hologram reconstruction corrected for measurements through layers with different refractive indices in digital in-line holographic microscopy |c Gonzalo H. Sendra, Sebastian Weisse, Stojan Maleschlijski, and Axel Rosenhahn |
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| 520 | |a Digital in-line holographic microscopy (DIHM) using point sources has been shown to be a versatile technique, especially for three-dimensional tracking of particles or microorganisms. However, the spherical source wave is altered when measurements are performed through layers with different refractive indices, such as water cuvettes. The situations where a layer of medium with a refractive index different than that of the predominant surrounding propagation medium (usually air) is situated behind or in front of the plane to be reconstructed are analyzed in detail, and a general approach for reconstruction under such circumstances is developed. The proposed refractive index correction is tested experimentally and compared to conventional reconstruction algorithms. Using 3D traces of swimming algal spores, the influence on the velocity calculation is also shown. | ||
| 650 | 4 | |a Diode pumped lasers | |
| 650 | 4 | |a Fast Fourier transforms | |
| 650 | 4 | |a First order optics | |
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| 650 | 4 | |a Refractive index | |
| 650 | 4 | |a Visible lasers | |
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