Asynchronous acquisition method based on Fourier transform spectrometer and Fourier transform spectrometer
A technology of Fourier transform and asynchronous acquisition, applied in the field of data processing, can solve problems such as avoiding crosstalk, and achieve the effect of avoiding signal crosstalk
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Embodiment 1
[0060] An asynchronous acquisition method based on a Fourier transform spectrometer, including a broadband light source and a laser light source, the methods include:
[0061] At the same time, the laser interference and the broadband optical interference signal of the standard are collected, and the spectrum is formed by Fourier transform, and the collected broadband optical interference is the first broadband optical interference W 0 , the collected laser interference is L 0 , calibrated synchronously and undergo Fourier transform to form spectrum F 0 ;
[0062] Turn off the laser light source, and collect the broadband optical interference signal of the standard object, wherein the collected broadband optical interference is the second broadband optical interference W 1 ;
[0063] Laser interference adjustment, the laser interference adjustment is performed through the synchronous variability between broadband light interference and laser interference, so as to obtain th...
Embodiment 2
[0074] On the basis of embodiment 1, this embodiment also includes calibration correction of broadband light:
[0075] use L 0 The adjusted L 1 Calibration for broadband light.
Embodiment 3
[0077] On the basis of the above embodiments, the difference between this embodiment and Embodiment 1 is that the laser interference adjustment method includes:
[0078] The first step is to calibrate the optical path such as laser interference and the first broadband optical interference W 1 ;
[0079] In the second step, the calibrated second broadband light interference W 1 Perform Fourier transform to obtain spectrum F 1 ;
[0080] The third step is to calculate the spectrum F 0 and spectrum F 1 The difference value D between the half-height center wavelength positions of the peaks;
[0081] The fourth step is to judge the difference value. When the difference value D is positive, gradually increase the value of the adjustment amount K with the set step size, and adjust the value of L 0 The time-domain subscript of the zero-crossing point is expanded by K times to obtain L 1 ; When the difference value is negative, gradually increase the value of the adjustment amou...
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