Square wave vector lock-in and amplification method for increasing signal-to-noise ratios of atomic frequency scale query signals
A technology of query signal and lock-in amplification is applied in the field of cesium atomic frequency standard, which can solve the problems of inability to stabilize the cesium atomic frequency standard, low signal-to-noise ratio, and large amplitude value error, so as to avoid complicated hardware devices and improve signal-to-noise. Compared with the effect of improving the accuracy
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Embodiment 1
[0034] Embodiment 1: Inquiry signal quadrature vector digital lock-in amplification with square wave modulation at 2 frequency points
[0035] (1) The Ramsey transition pattern of the 2-point frequency modulated cesium atomic clock is as follows image 3 shown. Take the resonant frequency of the cesium beam tube, that is, the frequency corresponding to the central peak is f 0 , when using 2-point frequency modulation, the 2 frequency points are respectively f 0 -F p1 and f 0 +F p1 , the corresponding signal amplitude is i 1 and i 2 . Among them, F p1 is a specified frequency offset, which is determined according to the specific parameters of the cesium atomic clock, where half of the frequency width of the central peak is taken.
[0036] (2) The modulated square wave signal input to the cesium beam tube is as follows: Figure 4 As shown, the frequency at f 0 -F p1 and f 0 +F p1 switch between. Here, each frequency point is 12.9ms, each cycle is 25.8ms, and lasts...
Embodiment 2
[0043] Embodiment 2: Inquiry signal quadrature vector digital lock-in amplification with square wave modulation at 4 frequency points
[0044] (1) The Ramsey transition pattern of the 4-point frequency modulated cesium atomic clock is as follows Image 6 shown. Take the frequency corresponding to the central peak as f 0 , when the 4-point frequency modulation method is adopted, the 4 frequency points are respectively f 0 -F p2 , f 0 -F p1 , f 0 +F p1 and f 0 +F p2 , the corresponding signal amplitude is i 3 i 1 i 2 and i 4 . Among them, F p1 , F p2 is the specified frequency offset, determined according to the specific cesium atomic clock parameters, here, F p1 Take half the frequency width of the central peak, F p2 Take the central peak frequency width.
[0045] (2) The modulated square wave signal input to the cesium beam tube is as follows: Figure 7 As shown, the frequency is first at f 0 -F p2 and f 0 +F p2 Switch between, each frequency point 12.9m...
Embodiment 3
[0051] Embodiment 3: Query Signal Orthogonal Vector Digital Lock-in Amplification with Square Wave Modulation at 3 Frequency Points
[0052] (1) Use the 3-point square wave at the central peak frequency point to modulate the Ramsey transition pattern of the cesium atomic clock as follows Figure 9 shown. Take the frequency corresponding to the central peak as f 0 , then the three frequency points are f 0 -F p1 , f 0 , f 0 +F p1 , the corresponding signal amplitude is i 1 i 3 and i 2 . Among them, F p1 Take half the frequency width of the central peak.
[0053] (2) The modulated square wave signal input to the cesium beam tube is as follows: Figure 10 As shown, the frequency is first at f 0 -F p1 and f 0 Switch between, each frequency point 12.9ms, each cycle 25.8ms, last 4 cycles; then f 0 +F p1 and f 0 Switch between, each frequency point 12.9ms, each cycle 25.8ms, last 4 cycles.
[0054] (3) The corresponding cesium beam tube output query signal is as fol...
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