Separation type Raman laser in full solid state
A Raman laser, split technology, applied in the field of lasers, can solve the problems of limiting laser output power level and beam quality, laser output energy level limitation, etc., and achieve excellent laser performance, high peak power, and large stimulated emission cross section. Effect
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Embodiment 1
[0042] According to Figure 1, a simple and compact all-solid-state Raman laser is produced. Diode laser used for side or end pumping, with a radius of curvature of 600mm, high transmittance to pump light of 808nm wavelength, high reflectivity to 1342nm and 1525nm wavelength laser cavity mirror 1, this is the input mirror; Nd 3+ :YVO 4 Crystal 2 is the laser gain medium; non-doped YVO 4 The crystal 5 is a Raman frequency shift medium; the acousto-optic Q-switch 3 is used to achieve quasi-continuous operation; a flat mirror (cavity mirror), which is highly reflective to the laser with the wavelength of 1342nm and partially transmits the laser with the wavelength of 1525nm, is the output mirror of the laser. 808nm laser diode pumped Nd 3+ :YVO 4 Crystal 2 generates laser light with a wavelength of 1342nm, which passes through undoped YVO 4 Crystal 5 produces Raman frequency shift from 1342nm fundamental frequency light to 1525nm wavelength Raman laser. Here, two mirror cavities are u...
Embodiment 2
[0044] According to Figure 2, a simple and compact all-solid-state Raman laser is produced. Diode laser for side-pumping, with a radius of curvature of 600mm, a cavity mirror 1 that is highly transparent to the pump light of 808nm wavelength and highly reflective to the laser of 1342nm wavelength, this is the input mirror; Nd 3+ :YVO 4 Crystal 2 is the laser gain medium; non-doped YVO 4 Crystal 3 is a Raman frequency shift medium; acousto-optic Q-switch 4 is used to achieve quasi-continuous operation; a flat mirror (cavity mirror), a faces 1342nm fundamental frequency light with high transparency, b faces 1342nm fundamental frequency light with high transparency, High reflection for 1525nm Raman laser; undoped YVO 4 The crystal is a Raman frequency-shifting medium; a flat mirror (cavity mirror), which is highly reflective to the 1342nm wavelength laser, and partially transmits the 1525nm wavelength laser, is the output mirror of the laser. 808nm laser diode pumped Nd 3+ :YVO 4 The...
Embodiment 3
[0046] According to Figure 3, an all-solid-state Raman laser with a three-mirror folded cavity was fabricated. Diode laser used for side or end pumping, with a radius of curvature of 600mm, high transmittance to pump light of 808nm wavelength, high reflectivity to 1342nm and 1525nm wavelength laser cavity mirror 1, this is the input mirror; Nd 3+ :YVO 4 Crystal 2 is the laser gain medium; non-doped YVO 4 The crystal is a Raman frequency-shifting medium; the acousto-optic Q-switch is used to achieve quasi-continuous operation; a plano-concave mirror, high reflection for the 1342nm fundamental frequency light and 1525nm Raman laser; non-doped YVO 4 Crystal 5 is a Raman frequency-shifting medium; a flat mirror (cavity mirror), which is highly reflective to the laser with a wavelength of 1342nm, partially transmits the laser with a wavelength of 1525nm, and is the output mirror of the laser. 808nm laser diode pumped Nd 3+ :YVO 4 Crystal 2 generates laser light with a wavelength of 134...
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