Output Stabilization of Wavelength-Swept Laser Based on Closed-Loop Control of Fabry–Pérot Tunable Wavelength Filter for Fiber-Optic Sensors

• Published in: Sensors (Basel, Switzerland) Switzerland), 2022-06, Vol.22 (12), p.4337
• Main Authors: Choi, Byeong Kwon, Ahn, Soyeon, Kim, Ji Su, Pagidi, Srinivas, Jeon, Min Yong
• Format: Article
• Language: English
• Subjects: Bragg gratings; closed-loop control; Communication; Domains; Electric potential; Fabry-Perot filters; Fabry–Pérot tunable wavelength filter; Feedback control; fiber laser; fiber-optic sensors; Function generators; Laser applications; Lasers; Light sources; Optics; Position measurement; Sensors; Signal processing; Stabilization; Temperature dependence; Tunable filters; Voltage; wavelength stabilization algorithm; wavelength-swept laser stabilization
• ISSN: 1424-8220; 1424-8220
• DOI: 10.3390/s22124337

The output of a wavelength-swept laser (WSL) based on a fiber Fabry–Pérot tunable filter (FFP-TF) tends to shift the peak wavelength due to external temperature or heat generated by the FFP-TF itself. Therefore, when measuring the output of WSL for a long time, it is very difficult to accurately measure a signal in the temporal domain corresponding to a specific wavelength of the output of the WSL. If the wavelength variation of the WSL output can be predicted through the peak time information of the forward scan or the backward scan from the WSL, the variation of the peak wavelength can be compensated for by adjusting the offset voltage applied to the FFP-TF. This study presents a successful stabilization method for peak wavelength variation in WSLs by adjusting the offset voltage of the FFP-TF with closed-loop control. The closed-loop control is implemented by measuring the deviation in the WSL peak position in the temporal domain using the trigger signal of the function generator. The feedback repetition rate for WSL stabilization was approximately 0.2 s, confirming that the WSL output and the peak position for the fiber Bragg grating (FBG) reflection spectrum were kept constant within ±7 μs at the maximum when the stabilization loop was applied. The standard deviations of WSL output and reflection peak positions were 1.52 μs and 1.59 μs, respectively. The temporal and spectral domains have a linear relationship; the ±7 μs maximum variation of the peak position corresponded to ±0.035 nm of the maximum wavelength variation in the spectral domain. The proposed WSL system can be used as a light source for temperature or strain-dependent sensors as it compensates for the WSL wavelength variation in applications that do not require a fast scanning rate.