A dual-wavelength laser based on stimulated Raman scattering of aqueous ethanol solution
A technology of stimulated Raman scattering and dual-wavelength lasers, which is applied to lasers, laser components, and lasers using scattering effects, etc., can solve the problem of limited optical frequency conversion crystal damage threshold, difficulty in obtaining high-energy laser pulses, and dual-wavelength lasers. The problem of large laser wavelength intervals achieves the effects of enhanced blood oxygen-carrying capacity, convenient experimental debugging, and flexible medium length.
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Embodiment 1
[0065] A dual-wavelength laser based on stimulated Raman scattering in ethanol aqueous solution, including a pump source 1, an aperture 2, a nonlinear crystal 3, a second color filter 4, a beam reduction system 5, and a first window sequentially arranged along the optical path Sheet 6, Raman box 7, second window 8, first color filter 9, first window 6, Raman box 7, and second window 8 are sealed and connected in turn, and Raman box 7 is filled with ethanol aqueous solution. Such as figure 1 shown.
[0066] The pump source 1 is a PY61 Nd:YAG mode-locked laser produced by Continuum Company, which outputs laser light with a wavelength of 1064 nm, a pulse width of 40 ps, and a repetition rate of 10 Hz.
[0067] Aperture 2 is a baffle with a circular aperture with a diameter of 6 mm.
[0068] The nonlinear crystal 3 is a KTP frequency doubling crystal, and the wavelength after frequency doubling is 532nm.
[0069] The second color filter 4 is coated with a dielectric film tha...
Embodiment 2
[0092] According to the dual-wavelength laser based on the stimulated Raman scattering of ethanol aqueous solution described in Embodiment 1, the difference is that the beam reduction system 5 is removed and the lens 10 is replaced.
[0093] The lens 10 is a biconvex lens or a plano-convex lens, which is used to increase the pump light power density incident on the Raman medium.
[0094] The structural representation of the dual-wavelength laser described in embodiment 2 is as Figure 7 shown.
Embodiment 3
[0096] According to the dual-wavelength laser based on the stimulated Raman scattering of ethanol aqueous solution described in embodiment 1, the difference is that the input mirror 11 is placed between the beam shrinkage system 5 and the first window 6, and the output is placed behind the second window 8. Mirror 12, forming a resonant cavity for the Raman laser.
[0097] The input mirror 11 is coated with a dielectric film with high transparency to 532nm laser and high reflection to 600-700nm laser.
[0098] The output mirror 12 is coated with a dielectric film that is highly reflective to 532nm laser and partially transparent to 600-700nm laser.
[0099] In this embodiment, the high reflection of the output mirror 12 to the 532nm laser can realize double-pass pumping, which improves the output energy and conversion efficiency of the dual-wavelength laser.
[0100] The structural representation of the dual-wavelength laser described in embodiment 3 is as follows Figure 8 s...
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