2016
DOI: 10.1016/j.optlastec.2016.01.025
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Distance measurement using frequency scanning interferometry with mode-hoped laser

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Cited by 26 publications
(3 citation statements)
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“…Therefore, the scanning stage will contribute 1.0 × 10 −6 L to the PI measurement uncertainty, as represented by the blue line in figure 8. Because the FIU and the RFI were illuminated by the same tunable laser source and acquired simultaneously by two BPs, the interference signals that are produced in just one wavelength scanning are correlated [24]. If the fringe counting method is absolutely accurate, the ratio of the two interference signals during one wavelength scanning will not change when a number of the signals are split.…”
Section: Uncertainty Evaluationmentioning
confidence: 99%
“…Therefore, the scanning stage will contribute 1.0 × 10 −6 L to the PI measurement uncertainty, as represented by the blue line in figure 8. Because the FIU and the RFI were illuminated by the same tunable laser source and acquired simultaneously by two BPs, the interference signals that are produced in just one wavelength scanning are correlated [24]. If the fringe counting method is absolutely accurate, the ratio of the two interference signals during one wavelength scanning will not change when a number of the signals are split.…”
Section: Uncertainty Evaluationmentioning
confidence: 99%
“…Furthermore, the larger the sweeping range, the smaller the corresponding synthesized wavelength, and the higher the ranging accuracy under the same accuracy of fringe counting. Fabry-Perot interferometer [20], highresolution saturated absorption spectra [21] and optical frequency comb [22] have been employed to calibrate the swept frequency range, and a range of 505 GHz was calibrated by the comb using a narrow band pass filter [23]. However, the external reference standards increase the complexity and cost of the system.…”
Section: Introductionmentioning
confidence: 99%
“…For a distance measurement system based on FSI, the measured distance L can be estimated by L = cΔΦ/(2π • B • n g ), where B is the optical frequency sweeping range of the laser, ΔΦ is the phase change of the interference signal, c is the speed of light in vacuum and n g is the group refractive index of air [6,7]. The theoretical measurement accuracy and precision are subject to the sweeping range and linearity of the laser source [8].…”
Section: Introductionmentioning
confidence: 99%