Method and device for realizing square wave quadrature demodulation of closed-loop resonant optical gyroscope
A quadrature demodulation and optical gyroscope technology, applied in the fields of optical sensing and signal detection, can solve problems such as phase fluctuation of the square wave signal to be demodulated, and achieve the effects of suppressing demodulation signal fluctuation, suppressing performance degradation, and improving accuracy
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Embodiment 1
[0093] Figure 9 This is the test result of the demodulation curve before and after square wave quadrature demodulation. The demodulation curve is obtained by scanning the center frequency of the laser. Figure 9 (a) is the demodulation curve without square wave quadrature demodulation; Figure 9 (b) is the demodulation curve under square wave quadrature demodulation, its working point θ 0 Set to π / 4rad. In the experiment, artificially set Δθ to 0, π / 20rad and π / 10rad. It can be found that when square wave quadrature demodulation is not used, such as Figure 9 As shown in (a), the slope of the demodulation curve will fluctuate with Δθ, so it is impossible to keep the slope of the demodulation curve at the maximum value; when the square wave quadrature demodulation method is adopted, as Figure 9 As shown in (b), the slope fluctuation of the demodulation curve is suppressed and almost kept near the maximum value.
Embodiment 2
[0095] To illustrate the necessity of optimizing the phase operating point when using square wave quadrature demodulation, Figure 10 The demodulation curve test comparison results when the operating point is set to 0 and π / 4rad are given. It can be found that when the operating point is set to 0, there is an obvious fluctuation around the resonance point, and when the operating point is set to π / 4rad, the fluctuation is suppressed.
Embodiment 3
[0097] Figure 11 The Allan variance analysis results of the test data of the gyroscope 1h output signal when the square wave quadrature demodulation method is used and the working points are set to 0 and π / 4rad respectively are given. The integration time is 0.1s and the sampling rate is 10Hz. according to Figure 11 According to the Allan variance analysis results, when the quadrature demodulation operating point is set to 0, the zero bias stability of about 11.9deg / h can be obtained, which is even better than what we have reported Figure 12 The test result shown without the square wave quadrature demodulation scheme is worse at about 7.1deg / h, which may be caused by the demodulation curve fluctuating near the resonance point under the non-ideal phase operating point. However, when the operating point is set to π / 4rad, a bias stability of about 6.0deg / h can be obtained. The bias stability is about Figure 12 The non-square-wave quadrature demodulation scheme shown yield...
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