Portable high-resolution optical fiber CARS microscopic excitation source device and implementation method
A high-resolution, excitation source technology, applied in the direction of measuring devices, optics, and analytical materials, can solve the problems of large and complex systems, slow tuning speed, and poor repeatability, and achieve improved spectral resolution, reliable spectral compression, and environmental resistance. Disruptive effect
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Embodiment 1
[0029] Example 1: Portable high-resolution optical fiber CARS micro-excitation source device
[0030] A portable high-resolution optical fiber CARS microscopic excitation source device and method, the specific implementation examples are as follows: the whole device consists of: femtosecond fiber laser light source 1, beam splitter 2, electronically controlled phase retarder 3, polarizer 4, Photonic crystal fiber 5, multimode fiber 6, single-mode fiber 7, electronically controlled delay line 8, beam combiner 9, output port 11, in specific implementation, the light source 1 is a femtosecond fiber laser light source, the pulse width is 100fs, the center The wavelength is from 600nm to 980nm, and the modulation frequency is within 100MHz.
[0031] The femtosecond laser pulse provided by the femtosecond fiber laser source has a pulse width of 60-150fs, a center wavelength of 600nm-1060nm, a repetition frequency of 50-200MHz, and an average power of 80mW-200mW;
[0032] The electr...
Embodiment 2
[0040] Embodiment 2: Generation method of portable high-resolution optical fiber CARS microscopic excitation source
[0041] The femtosecond laser pulse is generated by a femtosecond fiber laser, and passes through a beam splitter to generate two beams of femtosecond pulse light, which are used as pump light and Stokes light respectively. The Stokes light changes the polarization state after passing through the electronically controlled phase retarder, and then combines the analyzer to modulate the power of the pulsed laser. In the photonic crystal fiber, femtosecond pulsed light with different powers produces different optical soliton frequency shifts, realizing Fast and wide tuning, and then through the serial connection of multi-mode fiber and single-mode fiber, the chirp processing of Stokes light pulses is realized to compress the spectral width; the other beam of pump light is adjusted by an electronically controlled delay line to make it Synchronized with the Stokes lig...
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