A direct-detection Brillouin optical time-domain reflectometry (BOTDR) using an up-conversion photon-counting detector and an all-fiber structure Fabry–Perot scanning interferometer is demonstrated with shot-noise limited performance. Taking advantage of ultra-low noise equivalent power of the up-conversion photon-counting detector and high spectral resolution of the interferometer, the Brillouin spectra along a polarization maintaining fiber (PMF) are analyzed in the optical frequency domain directly. In contrast with heterodyne BOTDR, photon-counting BOTDR has better EM compatibility and faster speed in data processing. In experiments, using peak input power of 20dBm, temperature profile along a 9km PMF is retrieved according to the Brillouin shifts, with spatial/temporal resolution of 2m/15s. The precision is 0.7°C at the leading end and 1.2°C at the trailing end.
Fig. 1. System layout. EOM, electro-optic modulator; AWG, arbitrary waveform generator; EDFA, erbium doped fiber amplifier; C, circulator; PC, polarization controller; TCC, temperature controlled chamber; FFP-SI, fiber Fabry–Perot scanning interferometer; FBG, fiber Bragg grating; TDFA, thulium doped fiber amplifier; WDM, wavelength division multiplexer; SMF, single mode fiber; TEC, thermo-electric cooler; DM, dichroic mirror; SPF, short-pass filter; LPF, long-pass filter; and BPF, band-pass filter.
Fig. 2. (a) Brillouin spectra of unstrained PMF when the probe pulse lunched from the leading end. (b) Zoom-in image of (a) from 0 to 0.2 km. (c) Brillouin spectra when the probe pulse lunched from the trailing end. (d) Zoom-in image of (c) from 8.8 to 9 km.
Fig. 3. Nonlinear fitting of the raw data to Lorentz functions at different ranges. Residuals are relative to the peaks.
For the first time, to the best of our knowledge, a direct detection Brillouin optical time-domain reflectometry (BOTDR) is demonstrated for fast distributed dynamic strain sensing incorporating double-edge technique, time-division multiplexing technique and upconversion technique. In order to guarantee the robust stability of the system, the double-edge technique is implemented by using a convert single-channel FPI and a fiber- coupled upconversion single-photon detector, incorporating a time-division multiplexing method. The upconversion single-photon detector is adopted to upconvert the backscattering photons from 1548.1 nm to 863 nm, which is subsequently detected by a Silicon avalanche photodiode (Si-APD). In the experiment, dynamic strain disturbance up to 1.9 mε over 1.5 km of a polarization maintaining fiber is detected at a sampling rate of 30 Hz. An accuracy of ± 30 με and spatial resolution of 0.6 m are realized.
Fig. 1. Optical layout of the system. DFB, distributed feedback diode; EOM, electro-optic modulator; EDFA, erbium doped ?ber ampli?er; C, circulator; FBG, ?ber bragg grating; PMF, polarization-maintaining fiber; PC, polarization controller; FPI, Fabry-Perot interferometer; TCC, temperature controlled chamber; PMFC, polarization-main- taining ?ber coupler; TDFA, thulium doped fiber amplifier; WDM, wavelength division multiplexer; PPLN-W, periodically poled Lithium niobate waveguide; TEC, thermo-electric cooler; MMF, multimode fiber; IF, interferometer filter.
Fig. 2. (a) Retrieved strain results; (b) histogram distribution of the strain difference between the measured result and fitting result.