Device and method for inhibiting nonlinear scanning of laser of optical frequency domain reflectometer
A technology of optical frequency domain reflection and nonlinear scanning, which is applied in electromagnetic wave transmission systems, electrical components, transmission systems, etc., and can solve the problems of limiting the maximum test distance of optical frequency domain reflection technology and reducing the bandwidth of acquisition systems
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Embodiment 1
[0073] Embodiment 1. Device for suppressing the influence of laser nonlinear scanning of optical frequency domain reflectometer
[0074] Such as figure 1 As shown, the device includes:
[0075] Scanning laser 1: used to provide a light source for the optical frequency domain reflection system, and its optical frequency can be linearly scanned;
[0076] 1:99 optical beam splitter 4: the output light of the laser enters the first port 1 of the optical beam splitter, and is distributed from the second and third ports 2 and 3 to the additional interferometer 6 and main interferometer 18;
[0077] Additional interferometer 6: used for collecting and monitoring the optical frequency of the laser; including an isolator 19, a first 50:50 coupler 5, a first Faraday mirror 8 and a second Faraday mirror 9, a delay fiber 7 and a detector 2;
[0078] Isolator, preventing the reflected light from the second port of the first 50:50 coupler in the additional interferometer from entering t...
Embodiment 2
[0083] Embodiment 2. Method for suppressing the influence of laser nonlinear scanning of optical frequency domain reflectometer
[0084] Such as figure 2 Shown, the step of the inventive method is:
[0085] The first step is to perform preprocessing and bandpass filtering on the beat frequency signal collected by the additional interferometer to obtain the signal
[0086]
[0087] where x 0 , ξ 0 is the constant amplitude and phase of the beat frequency signal, The phase at n sample point time, and the phase at sample point time n-τ, respectively.
[0088] Step 2, perform Hilbert transform on the previous step signal (15)
[0089]
[0090] Step 3, divide the above (15) and (16), and use the arctangent operation to obtain the phase information of the additional interferometer beat frequency signal as image 3 Shown, and phase unwrapped:
[0091]
[0092] Step 4, normalize the phase information as Figure 4 As shown, since the optical frequency is proportional...
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