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For wavelengths above 1000 nm, the preferred OCT method utilizes wavelength-swept laser light sources, so-called swept sources, rather than a broadband light source and a spectrometer, because available detector arrays based on indium gallium arsenide have relatively low pixel numbers, which leads to a limited imaging depth range [ 19].
Wieser et al. demonstrated a 5.2 MHz A-scan rate FDML-type swept sources [ 16].
The method presented is especially suitable for those swept sources where by increasing the tuning speed, their coherence length diminishes.
With new semiconductor laser gain media, broadband swept sources spanning the 1060 nm window have become available.
Recent progress in the development of tunable lasers for SS-OCT lead to swept sources with coherence length longer than 1 cm [ 4, 5].
Continuing research focuses therefore on the development of high-performance swept sources for the 1060 nm range [ 20, 23, 25– 28].
Similar(44)
Abstract: Advances in swept source laser technology continues to increase the imaging speed of swept-source optical coherence tomography (SS-OCT) systems.
Light from a coherent swept source propagates in an all-fiber interferometric network made of a reference arm and a parallel connection of N sensing arms.
His research is focused on designing and developing the next generation of swept source optical coherence tomography systems with higher stability, faster speed, and less data bandwidth.
Choroidal thickness measured with swept source optical coherence tomography before and after vitrectomy with internal limiting membrane peeling for idiopathic epiretinal membranes.
To study the mean choroidal thickness and volume of the macula in eyes with angioid streaks using swept source optical coherence tomography (OCT) in the 1050-nm wavelength range.
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