2011
DOI: 10.1364/boe.2.001769
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True logarithmic amplification of frequency clock in SS-OCT for calibration

Abstract: With swept source optical coherence tomography (SS-OCT), imprecise signal calibration prevents optimal imaging of biological tissues such as coronary artery. This work demonstrates an approach using a true logarithmic amplifier to precondition the clock signal, with the effort to minimize the noises and phase errors for optimal calibration. This method was validated and tested with a high-speed SS-OCT. The experimental results manifest its superior ability on optimization of the calibration and improvement of … Show more

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Cited by 10 publications
(5 citation statements)
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“…Hence, each pair of OCT signal and clock signal were examined by the nearest neighbor check algorithm for crossing points, which can be performed according to methods reported in [45,46]. Next, the OCT data set was indexed by referencing these searched points prior to FFT process [47]. The axial resolution of the system is 12 µm in tissue and 16 µm in air, and the lateral resolution including the objective lens (Thorlabs.…”
Section: System Configuration Of Ss-octmentioning
confidence: 99%
“…Hence, each pair of OCT signal and clock signal were examined by the nearest neighbor check algorithm for crossing points, which can be performed according to methods reported in [45,46]. Next, the OCT data set was indexed by referencing these searched points prior to FFT process [47]. The axial resolution of the system is 12 µm in tissue and 16 µm in air, and the lateral resolution including the objective lens (Thorlabs.…”
Section: System Configuration Of Ss-octmentioning
confidence: 99%
“…However, this requires careful adjustment of the hardware components and the use of extra optical components in the interferometer introduces losses. In swept source OCT, the swept sources are often equipped with a supplementary k-clock [6] that adds to the cost of the source, consisting in an extra interferometer equipped with a photo-detector at least twice as fast as the highest frequency component to be detected in the main imaging interferometer from the maximum depth. It also requires a two input sophisticated digitizer.…”
Section: Real-time Operationmentioning
confidence: 99%
“…However, before the FFT, several preparatory signal processing steps are necessary, such as zero padding, spectral shaping, apodization, dispersion compensation, or data resampling. 5 Other techniques such as using an additional light source that produces several spectral lines in the region of interest of the spectrometer, 6 parametric iteration methods, 6 phase linearization techniques, 7,8 and automatic calibrations 9 have been proposed. 1 As all these steps can only be sequentially executed, the production of the B-scan images in real-time is limited.…”
Section: Introductionmentioning
confidence: 99%