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Enhancing Sun-pumped laser performance by a truncated fused silica elliptical pump cavity

机译:通过截短的熔融二氧化硅椭圆泵腔增强泵浦激光性能

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Sun-pumped lasers are useful for space and terrestrial applications. In terms of collection efficiency and beam quality, solar lasers still have a way to go to seriously compete with solar PV-cell diode-pumped solid-state lasers. The main challenges are the needs of both doubling the reported collection efficiency of 6.7W/m{sup}2 and improving the beam quality of today's solar lasers. To enhance the solar laser performance, a truncated fused silica elliptical pump cavity is proposed. With the first-stage parabolic mirror of 1.5m diameter, the solar power is both collected and concentrated into the 8mm diameter focal spot of 1250W. The input face of the truncated cavity is then mechanically positioned at the focal area of the parabolic mirror (Fig.1a). On passing through the air-fused silica interface, the concentrated rays of 60°rim-angle are refracted into the divergent rays of 36° rim-angle within the cavity machined from fused silica material. By both the reflections from a gold cavity reflector and the total internal reflections from the side faces of the cavity, the concentrated solar radiation is efficiently transferred from the first focal line, coplanar with the input face of the cavity, to the second focal line, where a laser rod is mounted and actively cooled by water. For the 1.0% Nd:YAG rod of 4mm diameter and 30mm length, a nearly symmetric absorbed flux profile is obtained (Fig.1 b, Fig.1 c). The absorbed flux peaks along the central core region of the rod, favouring the generation of TEM{sub}00 laser power.
机译:泵浦激光器可用于空间和地面应用。在收集效率和光束质量方面,太阳能激光器仍然有一种方法可以与太阳能光伏电池二极管泵浦固态激光器进行认真竞争。主要挑战是将报告的收集效率加倍,提高了当今太阳激光器的光束质量。为了增强太阳激光功率,提出了一个截短的熔融二氧化硅椭圆泵腔。通过直径为1.5米的第一级抛物面镜,太阳能均收集并集中到1250W的8mm直径焦点。然后机械地定位在抛物面镜的焦点区域(图1A)的截头腔的输入面。在通过燃气二氧化硅界面的情况下,60°Rim角的浓缩光线被折射到从熔融二氧化硅材料加工的腔内的36°边缘角的发散射线中。通过来自金腔反射器的反射和来自腔的侧面的总内部反射,浓缩的太阳辐射从第一焦线,与腔的输入面有效地从第一焦线转移到第二焦点线,在其中安装激光杆并主动被水冷却的地方。对于直径为4mm的1.0%ND:YAG棒,长度为30mm,获得了几乎对称的吸收通量曲线(图1b,图C)。沿杆的中央芯区域的吸收通量峰值,有利于产生TEM {SUB} 00激光功率的产生。

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