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    • 3. 发明授权
    • Semiconductor laser pumped multiple molecular gas lasers
    • 半导体激光泵浦多分子气体激光器
    • US5379315A
    • 1995-01-03
    • US980020
    • 1992-11-23
    • Richard A. Meinzer
    • Richard A. Meinzer
    • H01S3/0943H01S3/094H01S3/0941H01S3/223H01S5/40H01S3/22
    • H01S3/223H01S3/0941H01S3/094053H01S5/4012H01S5/4025
    • A gas laser cavity 44 comprises a first (pumped) molecular gas 52 and a second (lasing) molecular gas 52, such as Hydrogen Halides. The first gas is pumped by a plurality of semiconductor lasers 20 which provide light carried along optical fibers 26 that provide divergent light 32 to a collimating lens 34 that provides collimated light 36 to a focussing lens 38 that provides pumping light 40 which propagates within the gas laser cavity 44 in a zig-zag pattern, thereby providing a homogeneously excited medium and providing sufficient pathlength to give adequate absorption of the pump light. The pump light 40 has a wavelength within the absorption frequency band of the first gas 52 and a wavelength capable of pumping the first gas molecules from the ground state to an excited state. The energy of the first gas transfers to the second gas and lasing occurs in the second gas. Thus, the pumped gas may be selected based on absorption of the pumping light and the lasing gas selected based on the desired output lasing wavelength.
    • 气体激光腔44包括第一(泵浦)分子气体52和第二(激光)分子气体52,例如卤化氢。 第一气体被多个半导体激光器20泵送,这些半导体激光器20提供沿着光纤26携带的光,光纤26将发散光32提供给准直透镜34,准直透镜34将准直光36提供给聚焦透镜38,聚焦透镜38提供在气体内传播的泵浦光40 激光腔44以锯齿形图案,从而提供均匀激发的介质并提供足够的光程以给泵浦光充分吸收。 泵浦光40具有在第一气体52的吸收频带内的波长和能够将第一气体分子从基态泵浦到激发态的波长。 第一气体的能量转移到第二气体和激光发生在第二气体中。 因此,抽吸气体可以基于基于期望的输出激光波长选择的泵浦光和激光气体的吸收来选择。
    • 6. 发明授权
    • Laser oscillator provided with blower
    • 激光振荡器配有鼓风机
    • US09590380B2
    • 2017-03-07
    • US15040121
    • 2016-02-10
    • FANUC CORPORATION
    • Akihiko Nishio
    • H01S3/22H01S3/036H01S3/134H01S3/106H01S3/0943H01S3/104H01S3/041
    • H01S3/036H01S3/041H01S3/0943H01S3/104H01S3/1067H01S3/134H01S3/22
    • There was the problem that the pressure of the laser medium rises from the target value by the heat when generating laser light. The laser oscillator includes a controller, laser medium flow path, resonator part, blower, pressure detecting part, laser medium supply-exhaust part, and temporary stop command part. The controller controls the resonator part to stop to generate laser light if a temporary stop is commanded, controls the blower 18 to slow the rotational speed of the blower from the first rotational speed to the second rotational speed, and controls the laser medium supply-exhaust part so that the pressure is the second target value lower than the pressure at the time when the rotational speed of the blower is the second rotational speed.
    • 存在当产生激光时激光介质的压力从目标值通过热量升高的问题。 激光振荡器包括控制器,激光介质流路,谐振器部分,鼓风机,压力检测部分,激光介质供给排气部分和临时停止命令部分。 如果命令临时停止,控制器控制谐振器部分停止产生激光,控制鼓风机18将鼓风机的旋转速度从第一转速减慢到第二转速,并控制激光介质供给排气 使得压力是比鼓风机的转速为第二转速时的压力低的第二目标值。
    • 8. 发明申请
    • CO2 laser
    • CO2激光器
    • US20130003775A1
    • 2013-01-03
    • US13385698
    • 2012-03-02
    • Robert Neil Campbell
    • Robert Neil Campbell
    • H01S3/0943
    • H01S3/1616H01S3/094003H01S3/094096H01S3/0941H01S3/2232H01S3/2308H01S3/2375H01S3/2391
    • Efficient laser diode excited Thulium (Tm) doped solid state systems, directly matched to a combination band pump transition of Carbon Dioxide (CO2), have matured to the point that utilization of such in combination with CO2 admits effectively a laser diode pumped CO2 laser. The laser diode excited Tm solid state pump permits Continuous Wave (CW) or pulsed energy application. Appropriate optical pumping admits catalyzer free near indefinite gas lifetime courtesy of the absence of significant discharge driven dissociation and contamination. As a direct consequence of the preceding arbitrary multi isotopologue CO2, symmetric and asymmetric, gas mixes may be utilized without significant degradation or departure from initial mix specifications. This would admit, at raised pressure, a system continuously tunable from ˜9 μm to ˜11.5 μm, or sub picosecond amplification. This methodology offers advantages in regards scalability, pulse energy and power over alternative non linear conversion techniques in access to this spectral region.
    • 激发二极管激光二极管激发的钍(Tm)掺杂的固态系统直接与二氧化碳(CO2)的组合带泵转换相匹配,已经成熟到与二氧化碳的结合使用有效地允许激光二极管泵浦CO2激光器。 激光二极管激光Tm固态泵允许连续波(CW)或脉冲能量应用。 适当的光泵浦允许在无限期气体寿命期间自由的催化剂,由于没有显着的放电驱动的解离和污染。 作为上述任意多同位素二氧化碳的直接后果,可以使用对称和不对称气体混合物,而不会显着降低或偏离初始混合物规格。 这将承认,在升高的压力下,系统可以从〜9μm连续调节到〜11.5μm,或者是皮秒级放大。 该方法在可访问该光谱区域时在可扩展性,脉冲能量和功率方面提供了优于替代非线性转换技术的优点。