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首页> 外文期刊>Journal of the Optical Society of America, B. Optical Physics >Modeling of supersonic diode pumped alkali lasers
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Modeling of supersonic diode pumped alkali lasers

机译:超声波二极管泵浦碱金属激光器的建模

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3D computational fluid dynamics (CFD) modeling of supersonic diode pumped alkali lasers (DPALs), taking into account fluid dynamics and kinetic processes in the lasing medium, is reported. For a supersonic Cs DPAL with laser section geometry and resonator parameters similar to those of the 1-kW flowing-gas subsonic Cs DPAL [Quantum Electron. 42, 95 (2012)] the maximum achievable output power, similar to 7 kW, is 25% higher than that achievable in the subsonic case. Comparison between semi-analytical and 3D CFD models for Cs shows that the latter predicts much higher maximum achievable output power than the former. Optimization of the laser parameters using 3D CFD modeling shows that very high power and optical-to-optical efficiency, 35 kW and 82%, respectively, can be achieved in a Cs supersonic device pumped by a collimated cylindrical (0.5 cm diameter) beam. Application of end pumping or transverse pumping by collimated rectangular (large cross section similar to 2-4 cm(2)) beam makes it possible to obtain even higher output power, > 250 kW, for similar to 350 kW pumping power. The main processes limiting the power of Cs supersonic DPAL are saturation of the D-2 transition and large similar to 40% losses of alkali atoms due to ionization, whereas the influence of gas heating is negligibly small. For supersonic K DPAL, both gas heating and ionization effects are shown to be unimportant and the maximum achievable power, similar to 40 kW and 350 kW, for pumping by a similar to 100 kW cylindrical and similar to 700 kW rectangular beam, respectively, are higher than those achievable in the Cs supersonic laser. The power achieved in the supersonic K DPAL is two times higher than for the subsonic version with the same resonator and K density at the gas inlet, the maximum optical-to-optical efficiency being 82%. The power of the mechanical pump required for closed-cycle operation of supersonic DPALs was estimated for constant and variable area ratio diffusers. The nucleation rate of the alkali atoms during supersonic expansion was calculated and found to be negligible. (C) 2015 Optical Society of America
机译:报告了超声二极管泵浦碱金属激光器(DPAL)的3D计算流体动力学(CFD)建模,其中考虑了激光介质中的流体动力学和动力学过程。对于超音速Cs DPAL,其激光截面的几何形状和谐振器参数类似于1kW流动气体亚音速Cs DPAL [量子电子。 42,95(2012)]的最大可达到输出功率,类似于7 kW,比亚音速情况下可达到的输出功率高25%。 Cs的半解析CFD模型与3D CFD模型之间的比较表明,后者预测的最大可实现输出功率要比前者高得多。使用3D CFD建模优化激光参数显示,在由准直圆柱(直径为0.5 cm)的光束泵浦的Cs超声设备中,可以分别实现35 kW和82%的非常高的功率和光学效率。通过准直矩形光束(大横截面类似于2-4 cm(2))应用末端泵浦或横向泵浦,可以获得更高的输出功率,> 250 kW,类似于350 kW的泵浦功率。限制Cs超声DPAL功率的主要过程是D-2跃迁的饱和以及由于电离而导致的碱原子损失接近40%,而气体加热的影响则可以忽略不计。对于超音速K DPAL而言,气体加热和电离效应均不重要,而分别通过类似100 kW的圆柱形和类似700 kW的矩形光束进行抽运的最大可达到功率(类似于40 kW和350 kW)为比Cs超音速激光器所能达到的更高。在具有相同谐振器和气体进口处的K密度的情况下,超音速K DPAL的功率是亚音速KDPAL的两倍,最大光学效率为82%。对于恒定和可变面积比的扩散器,估计了超声波DPAL的闭环运行所需的机械泵的功率。计算了超声膨胀过程中碱原子的成核速率,发现该速率可以忽略不计。 (C)2015年美国眼镜学会

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