2015
DOI: 10.1007/s10043-015-0112-7
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Beam propagation analysis on thickness measurements in quantitative phase microscopy

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“…Now, to obtain the phase-map of each pixel, probe interferograms reflected from a trapped RBC were captured at a CCD camera and analysed by algorithms written in MATLAB. No reflection can occur from the intermediate cytoplasmic medium because it is transparent for visible wavelength of probe light (632 nm) thereby assuming no wavefront aberration from phase object (RBC) [80]. Total OPD between two co-propagating reflected interferograms: one from the top surface and other from the bottom surface of RBC (after transmission from the top surface) is twice the thickness of discotic RBC (0.9 µm -2.5 µm) i.e., 1.8 µm -5µm.…”
Section: Role Of Arbitrary Intensity Profile Beam In Trapping and mentioning
confidence: 99%
“…Now, to obtain the phase-map of each pixel, probe interferograms reflected from a trapped RBC were captured at a CCD camera and analysed by algorithms written in MATLAB. No reflection can occur from the intermediate cytoplasmic medium because it is transparent for visible wavelength of probe light (632 nm) thereby assuming no wavefront aberration from phase object (RBC) [80]. Total OPD between two co-propagating reflected interferograms: one from the top surface and other from the bottom surface of RBC (after transmission from the top surface) is twice the thickness of discotic RBC (0.9 µm -2.5 µm) i.e., 1.8 µm -5µm.…”
Section: Role Of Arbitrary Intensity Profile Beam In Trapping and mentioning
confidence: 99%