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Frequency-modulated continuous wave laser interferometry technology has broad application prospects in modern industrial production due to its advantages of large dynamic range, high precision, and high reliability. The frequency-modulated continuous wave laser is coupled with the Fabry-Perot interferometer in the optical field through optical fiber devices. The signal light and reference light of the interferometer propagate along the same optical fiber arm, which is extremely sensitive to displacement information. The measurement information can be obtained by demodulating the beat signal generated when the reference signal interferes with the measurement signal. In phase demodulation, the extreme point position of the beat frequency signal in one cycle is converted into a change in the initial phase to achieve displacement demodulation. But a beat frequency signal is a kind of sine signal with low signal noise, unequal amplitude, and frequency. It needs signal preprocessing to facilitate the subsequent extreme point location. Determining the precise position of the peak is the key problem in displacement demodulation.
Aiming at the demodulation problem of frequency modulation continuous wave interference beat frequency signal, this paper applies the centroid method to the field of the beat frequency signal demodulation and proposes a phase demodulation algorithm based on the centroid peak finding method. Compared with the existing phase demodulation algorithm, the algorithm does not need amplitude correction. After smooth filtering and minimum point positioning of the signal, the peak point position of the beat frequency signal can be accurately obtained by the centroid method, and the displacement amount can be obtained after phase demodulation according to this peak point position. A frequency-modulated continuous wave interferometric ranging system was constructed, and test experiments were carried out. The random error distribution of the displacement is verified when the length of the F-P cavity is fixed, and the standard deviation of the error is 2.18 nm. In order to compare the centroid peak-finding method proposed in this paper with the conventional zero-crossing detection method, the displacement random error of the two methods is obtained by using the built frequency modulated continuous wave ranging system with fixed different distances, and its standard deviation is calculated. Experimental results show that the measurement error of the method proposed in this paper is reduced by 49% compared to the traditional zero-crossing detection method. It has important research significance in the field of laser interferometry and has broad application prospects in the field of precision measurement.
Frequency relationship between reference wave and signal wave in sawtooth wave modulation
Flow chart of phase demodulation algorithm based on zero-crossing detection method
Beat signal peak clipping
Flow chart of the phase demodulation algorithm based on centroid peak-finding method
Phase error and displacement error corresponding to 10~60 dB signal to noise ratio. (a) Zero-crossing detection method; (b) Centroid peak-finding method
Schematic diagram of a frequency-modulated continuous-wave laser interference displacement sensor
Physical drawing of FMCW interferometric displacement measurement system
Beat signal and sawtooth signal acquired. (a) Sawtooth signal; (b) Beat signal
Random error and distribution of displacement when the length of the F-P cavity is 44 mm fixed by zero-crossing detection method. (a) Random error of displacement fixed distance; (b) Random error distribution
The random error and distribution of displacement when the length of the F-P cavity is 44 mm fixed by the centroid peak-finding method. (a) Random error of displacement fixed distance; (b) Random error distribution
Comparison of the standard deviation of displacement random error between zero-crossing detection method and centroid peak-finding method when F-P cavity length is different