不同泵送几何形状和不同流速下流动气体dpal的三维CFD建模

E. Yacoby, K. Waichman, O. Sadot, B. Barmashenko, S. Rosenwaks
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引用次数: 2

摘要

利用精确的三维计算流体动力学模型,考虑温度升高和碱原子电离损失的影响,研究了将流动气体二极管泵浦碱激光器(DPALs)放大到兆瓦级功率的问题。对Cs和K激光器的最大可达功率和光束质量进行了估计。我们考察了流速和马赫数M对亚音速和超音速激光器最大可达功率的影响。对于M = 0.2 ~ 3的Cs DPAL器件,输出功率仅随M的增加而增加约20%,这意味着超音速工作模式相对于亚音速只有很小的优势。相比之下,K DPALs可实现的功率强烈依赖于M,当M从0.2增加到4时,输出功率增加了~100%,显示出超声速器件相对于亚音速器件的相当大的优势。在Cs和K DPALs中,功率随M增大的原因是由于流动系统中气体膨胀导致温度降低。然而,K激光器的功率增长远大于Cs器件,这主要是由于2P态的精细结构分裂要小得多(K为~58 cm-1, Cs为~554 cm-1),这导致K DPALs的温度下降效应要强得多。对于相同矩形截面梁的泵浦,端泵浦与横向泵浦的对比表明,泵浦的几何形状不影响输出功率。然而,横向泵浦DPALs的输出光束强度在激光束截面上存在强烈的不均匀性,导致输出光束强度均匀的端泵浦几何形状在远场具有更高的亮度和更好的光束质量。
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3D CFD modeling of flowing-gas DPALs with different pumping geometries and various flow velocities
Scaling-up flowing-gas diode pumped alkali lasers (DPALs) to megawatt class power is studied using accurate three-dimensional computational fluid dynamics model, taking into account the effects of temperature rise and losses of alkali atoms due to ionization. Both the maximum achievable power and laser beam quality are estimated for Cs and K lasers. We examined the influence of the flow velocity and Mach number M on the maximum achievable power of subsonic and supersonic lasers. For Cs DPAL devices with M = 0.2 - 3 the output power increases with increasing M by only ~20%, implying that supersonic operation mode has only small advantage over subsonic. In contrast, the power achievable in K DPALs strongly depends on M. The output power increases by ~100% when M increases from 0.2 to 4, showing a considerable advantage of supersonic device over subsonic. The reason for the increase of the power with M in both Cs and K DPALs is the decrease of the temperature due to the gas expansion in the flow system. However, the power increase for K lasers is much larger than for the Cs devices mainly due to the much smaller fine-structure splitting of the 2P states (~58 cm-1 for K and ~554 cm-1 for Cs), which results in a much stronger effect of the temperature decrease in K DPALs. For pumping by beams of the same rectangular cross section, comparison between end-pumping and transverse-pumping shows that the output power is not affected by the pump geometry. However, the intensity of the output laser beam in the case of transverse-pumped DPALs is strongly non-uniform in the laser beam cross section resulting in higher brightness and better beam quality in the far field for the end-pumping geometry where the intensity of the output beam is uniform.
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