研究目的
To demonstrate a polarimetric fiber vibration sensor based on a polarization-diversified loop (PDL) with short polarization-maintaining photonic crystal fiber (PM-PCF) as a sensor head and investigate the dependence of its frequency response on the sensing fiber length.
研究成果
The short sensor head can provide higher normalized sensitivity, i.e., better signal to noise ratio, at frequencies higher than the resonance frequency, in addition to convenience of installation and insensitivity to external perturbations, in a PDL-based PM-PCF vibration sensor. The phase shift per unit strain and the minimum detectable strain perturbation were measured as ~0.377 mrad/με and ~0.16 nε/Hz1/2 at 2000 Hz for ~6-cm-long PM-PCF, respectively.
研究不足
The study is limited to the investigation of the frequency response of the sensor based on the length of the PM-PCF segment. The practical application may be constrained by the need for optimization of the operating point and the influence of external perturbations.
1:Experimental Design and Method Selection:
The sensor is composed of a Sagnac birefringence interferometer (SBI) based on a PDL, a laser diode (LD), and a photodetector (PD). The SBI is constructed using a fiber-pigtailed four port PBS, a fiber-pigtailed HWP, a fiber-pigtailed QWP, and PM-PCF.
2:Sample Selection and Data Sources:
Two kinds of PM-PCF segments with fiber lengths of ~6 and ~10 cm were employed.
3:List of Experimental Equipment and Materials:
Polarization beam splitter (PBS), PM-PCF, quarter-wave plate (QWP), half-wave plate (HWP), laser diode (LD), photodetector (PD), piezoelectric transducer (PZT), function generator, oscilloscope.
4:Experimental Procedures and Operational Workflow:
The frequency response was examined over 1–3000 Hz using a PZT to apply single-frequency vibration to the sensor head. The output power of the SBI was converted into voltage signals by the PD, and temporal changes in the output voltage of the PD were monitored by the oscilloscope.
5:Data Analysis Methods:
The frequency response of the fabricated sensor was measured at a frequency range from 1 to 3000 Hz. The signal amplitudes were normalized for comparison of two frequency responses.
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