2018
DOI: 10.1364/oe.26.003772
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Four dimensional phase unwrapping of dynamic objects in digital holography

Abstract: We present a new four-dimensional phase unwrapping approach for time-lapse quantitative phase microscopy, which allows reconstruction of optically thick objects that are optically thin in a certain temporal point and angular view. We thus use all four dimensions of the dynamic quantitative phase profile acquired, including the angular dimension and the temporal dimension, in addition to the x-y dimensions. We first demonstrate the capabilities of this algorithm on simulative data, enabling the quantification o… Show more

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Cited by 11 publications
(10 citation statements)
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“…According to the method in this paper, the cytoplasmic RI n1 can be calculated according to formulas ( 9), (10), and (13). The RI n2 of the nucleus can be calculated according to formulas (11), (12), and (13). Eqs.…”
Section: Simulation Experimentsmentioning
confidence: 99%
See 1 more Smart Citation
“…According to the method in this paper, the cytoplasmic RI n1 can be calculated according to formulas ( 9), (10), and (13). The RI n2 of the nucleus can be calculated according to formulas (11), (12), and (13). Eqs.…”
Section: Simulation Experimentsmentioning
confidence: 99%
“…The direct thickness measurement method measures geometric thickness by different imaging methods, such as atomic force microscopy [4], confocal reflectance microscopy [5], and the combination of a confocal fluorescence microscopy and phase microscopy [6], but these methods increase the complexity of the combined system and may damage cells. Tomographic phase microscopy method (TPM) uses the phase [7][8][9][10][11] to image objects from different perspectives. After digitizing the phase map, it is possible to decouple two-dimensional information and obtain a three-dimensional distribution of the RI of the cells, but the method requires multiple measurements and extensive calculations for many angles.…”
Section: Introductionmentioning
confidence: 99%
“…In optical multiplexing [11][12][13][14][15][16][17][18][19][20][21][22][23][24][25][26][27][28][29][30], multiple sample and reference beam pairs with different 𝜃 𝑥 and 𝜃 𝑦 combinations are projected onto the digital camera simultaneously, each of which creating an off-axis hologram with a different interference fringe direction that positions one wavefront in the SFD without overlapping other terms. The simultaneous projection of all beams on the camera may create unwanted interference between nonmatching pairs.…”
Section: Optical Multiplexingmentioning
confidence: 99%
“…Various basic architectures have been demonstrated for optical multiplexing. These include multiplexing two holograms by positioning two complex wavefronts in two orthogonal directions [11][12][13][14][15][16][17][18][19][20][21], which can be generalized to multiplexing three [22][23][24][25], four [26][27][28], five [29], or even six holograms [30], all without SFD overlap.…”
Section: Optical Multiplexingmentioning
confidence: 99%
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