Method and system for eliminating double-optical-comb frequency spectrum aliasing
A spectrum aliasing and dual-comb technology, which is applied in the radio wave measurement system, electromagnetic wave re-radiation, utilization of re-radiation, etc., can solve the problem of the unavailability of the dual-comb system, the great influence of the deviation frequency change, the limitation of repetition frequency and deviation Frequency adjustable range and other issues to achieve the effect of improving the ability of long-term stable measurement, reducing the requirements of the use environment, and avoiding dead zones
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Embodiment 1
[0059] Based on the above inventive concept, such as Figure 4 As shown, the laser ranging system for eliminating dual-comb spectral aliasing provided by this embodiment includes a first optical comb 1, a second optical comb 2, a reference mirror 3, a measuring mirror 4, a first bandpass filter 5, A second band-pass filter 6 , a first detector 7 , a second detector 8 , a first low-pass filter 9 , a second low-pass filter 10 and a signal processor 11 .
[0060] The signal light pulse sent by the first optical comb 1 is split by the first beam splitter 12, and one beam of light is incident on the reference mirror 3, and the other beam of light is incident on the measuring mirror 4, and the light reflected by the reference mirror 3 and the measuring mirror 4 passes through the first The beam splitter 12 exits to the second beam splitter 13;
[0061] The second optical comb 2 emits local oscillator light pulses and enters the second beam splitter 13 and interferes with the light ...
Embodiment 2
[0071] This embodiment also provides a laser ranging method for eliminating dual-comb spectrum aliasing, including the following:
[0072] The signal light pulse sent by the first optical comb 1 passes through the first beam splitter, one beam of light is incident on the reference mirror 3, the other beam of light is incident on the measuring mirror 4, and the light reflected by the reference mirror 3 and the measuring mirror 4 passes through the first beam splitter 12 emerges to the second beam splitter 13;
[0073] The second optical comb 2 emits a local oscillator light pulse that is incident on the second beam splitter 13 and interferes with the light emitted by the first beam splitter 12;
[0074] A part of the light emitted by the second beam splitter 13 is obtained through the first band-pass filter 5 to obtain frequency components in a certain frequency range; another part of the light emitted by the second beam splitter 13 is obtained by the second band-pass filter 6 ...
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