2012
DOI: 10.1364/ol.37.002190
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Full off-axis red-green-blue digital holographic microscope with LED illumination

Abstract: We developed a new full off-axis red-green-blue (RGB) digital holographic microscope with an LED illumination. A decisive advantage of the use of LED illumination is a large image quality improvement due to its partially coherent nature. The off-axis configuration enables the fast recording of the holographic data in each spectral channel. The digital holographic refocusing and the optical phase map computation are successfully demonstrated. The multiwavelength operation provides a significant improvement of t… Show more

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Cited by 63 publications
(33 citation statements)
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“…To overcome the coherent noise, coherent lasers are replaced by light sources of partial coherence (partial temporal coherent light or partial spatial coherent light) [21][22][23][24][25][26][27][28][29][30][31][32][33][34][35][36][37]. Nevertheless, a light emitting diode (LED) as a light source for DHMs has not yet been fully exploited [30][31][32][33][34][35][36][37]. The principle in LED light source (as well as with other short time coherence light source) illuminated DHM is optical path length compensation between an object and reference arms, which is achieved by using optics pairs in both arms, as in a Michelson or a Mach-Zehnder interferometer [32][33][34][35][36][37].…”
Section: Introductionmentioning
confidence: 99%
“…To overcome the coherent noise, coherent lasers are replaced by light sources of partial coherence (partial temporal coherent light or partial spatial coherent light) [21][22][23][24][25][26][27][28][29][30][31][32][33][34][35][36][37]. Nevertheless, a light emitting diode (LED) as a light source for DHMs has not yet been fully exploited [30][31][32][33][34][35][36][37]. The principle in LED light source (as well as with other short time coherence light source) illuminated DHM is optical path length compensation between an object and reference arms, which is achieved by using optics pairs in both arms, as in a Michelson or a Mach-Zehnder interferometer [32][33][34][35][36][37].…”
Section: Introductionmentioning
confidence: 99%
“…12,31 Although in the demonstration we adopt a He-Ne laser as our light source to simplify the optical system, DAOLCI can be directly applied to diode laser or superluminescent diode by use of low-coherence DH. [32][33][34][35][36] Compared to the classical AO confocal imaging modality, DAOLCI does not require certain hardware pieces, such as a Shack-Hartmann wavefront sensor, deformable mirror, and He closed-loop feedbacks, and also opens the possibilities of adopting computational AO techniques [19][20][21] to correct for the aberration. As all the conventional AO ophthalmoscopes adopt, we have assumed the aberration happens at or close to the pupil.…”
Section: Discussionmentioning
confidence: 99%
“…Also, coherent noise seems inevitable if laser is used as the light source. This can be addressed by use of low coherent light source [21,22,25]. …”
Section: Discussionmentioning
confidence: 99%