Author Affiliations
1Ultrafast Laser Laboratory, Key Laboratory of Opto-electronic Information Science and Technology of Ministry of Education, School of Precision Instruments and Opto-electronics Engineering, Tianjin University, Tianjin 300072, China2Institute of Spacecraft System Engineering, China Academy of Space Technology, Beijing 100094, China3National Institute of Metrology, Beijing 100029, Chinashow less
Fig. 1. Configuration of all-PM NALM mode-locked fiber laser. WDM, 980/1550 nm wavelength division multiplexer; PBC, polarization beam coupler; Col., collimator; FR, Faraday rotator; QWP, quarter waveplate. The FR and QWP form the nonreciprocal phase shifter. Optical spectra of two mode-locked lasers. Blue line, laser 1; red line, laser 2.
Fig. 2. Working principle of ASOPS. Two laser sources that have slightly different repetition frequency rates ( and ) are used. Every period , the LO will take a complete sampling signal of the SL pulse via sum-frequency generation (SFG).
Fig. 3. Experimental setup of the robust LIDAR system. Two free-running all-PM lasers with slightly different repetition rates (∼80.267 MHz, ∼82.269 MHz) are used as the laser sources. An FC/PC connector having 4% Fresnel reflection at the surface and a hollow retroreflector are used as the reference and target mirror, respectively. The absolute distance between the reference and target mirrors is obtained through optical intensity cross-correlation between the reflected SL and LO pulses. Note that the telescope is focal length adjustable. SL, single laser; LO, local oscillator; ISO, isolator; HWP, half-waveplate; Col., collimator; Ref., reference mirror; Tar., target mirror; PBS, polarization beam splitter; PPKTP, periodically poled ; APD, avalanche photo-detector; LPF, low pass filter.
Fig. 4. (a) Absolute distance measurement results of the femtosecond absolute ranger compared with the standard interferometers. (b) Residuals of measured distance versus truth data from standard interferometers at the NIM. The averaging period for the TOF measurement is 500 ms.
Fig. 5. Allan deviations at absolute distances of 30 and 60 m. The measurement accuracy increases with the increase of averaging time and reaches less than 1 μm at 1 s averaging time.
Fig. 6. Residuals of measured distance after the Kalman filter compared with the standard interferometers. The residuals and deviations are less than 3 μm, while the update rate is 200 Hz.
Parameters | Laser 1 | Laser 2 |
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Pump power | 218.7 mW | 220.3 mW | Output1 power | 6.20 mW | 7.69 mW | Output2 power | 15.58 mW | 14.66 mW | Repetition rate | 80.267 MHz | 80.269 MHz | | 1569.4 nm | 1571.8 nm | FWHM | 13.2 nm | 11.8 nm |
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Table 1. Output Parameters of Two Lasers