A Supercontinuum Light Source and Coherent Anti-Stokes Raman Scattering Imaging System
A supercontinuum light source and supercontinuum technology, applied in the field of supercontinuum light source and coherent anti-Stokes Raman scattering imaging system, can solve the problem of poor time-spectrum consistency of supercontinuum light source and achieve good flatness And the effects of continuity, wide application, and relatively small time delay
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Embodiment 1
[0027] Such as figure 1 As shown, the supercontinuum light source provided by the embodiment of the present invention includes a laser 1 for generating laser pulses, and the full positive dispersion photonic crystal fiber 2 is pumped by the laser pulses to generate the supercontinuum. Wherein, the laser generally adopts a femtosecond laser, and the laser pulse is a femtosecond pulse. The supercontinuum generated in this way maintains a single pulse in the time domain, has better flatness and continuity in the frequency domain, and has a higher spectral power density. At the same time, the relative time delay between the spectral components of different frequencies is small, the time-spectrum consistency is good, and the spectral range is wide.
[0028] Generally, the supercontinuum light source also includes a continuously variable attenuator, a beam expander 3, and a coupling objective that are sequentially arranged along the propagation direction of the laser pulse; wherein, th...
Embodiment 2
[0036] Figure 5 The architecture of a coherent anti-Stokes Raman scattering imaging system provided by an embodiment of the present invention is shown, and the details are as follows. The system includes a femtosecond laser 1, a spectroscopic device 21, a conversion device 22, a delay device 23, a collinear focusing device 25 and an imaging device 24. Wherein, the femtosecond laser 1 is used to generate ultrashort laser pulses. The spectroscopic device 21 is used to generate a first ultrashort laser pulse and a second ultrashort laser pulse from the ultrashort laser pulse. The conversion device 22 is used to convert the first ultrashort laser pulse into a supercontinuum, wherein the supercontinuum is used as pump light and Stokes light acting on the sample to generate coherent phonons. . The delay device 23 is used to adjust the time for the second ultrashort laser pulse to reach the sample, wherein the delayed second ultrashort laser pulse is used as the probe light. The c...
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