皮秒激光冲击金属的残余能量测量

E. Loktionov, E. Sharaborova, D. Sitnikov
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引用次数: 0

摘要

剩余能量或热耦合系数表示用于加热目标的激光脉冲能量的比例。高的剩余能量率导致低的冲击效率,有时会导致不希望的影响,如相变和化学反应。在纳米和飞秒激光照射下对其测量的实验工作不多,但仍有发现,而皮秒范围的研究较少。后者很有趣,因为热耦合效应接近超短冲击,而激光器的效率、复杂性和价格更接近纳秒器件。我们使用量热计来评估通过聚焦和非聚焦辐照目标的热通量。我们获得的铝在1064 nm, 71 ps, 15 Hz辐照下的数据显示,剩余能量率高于已发表的来源:比100 ps时计算的高2.5-3倍,比纳米和飞秒冲击的实验评估高1.25倍。我们认为这种差异可能是由于反复撞击后目标的实际吸收率的变化,光束的空间形状(均匀或高斯)以及所使用的实验方法(目标温度或通过热流)。所获得的结果非常新颖,对于热耦合的正确建模以及使用重复脉冲皮秒冲击从实验室到实际系统的充分过渡具有重要意义。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Residual Energy Measurement at Picosecond Laser Impact on Metals
Residual energy or thermal coupling coefficient shows what fraction of laser pulse energy is spent for target heating. High residual energy rates lead to low impact efficiency and sometimes to unwanted effects like phase transitions and chemical reactions. Experimental works on its measurement under nano- and femtosecond laser irradiation are not numerous but still can be found, while picosecond range is poorly studied. The latter is interesting since thermal coupling effects are close to ultrashort impact, while lasers efficiency, complexity, and price are closer to nanosecond devices. We used a calorimeter to evaluate heat flux through a target for focused and non-focused irradiation. Our data obtained for aluminum irradiated at 1064 nm, 71 ps, 15 Hz show higher residual energy rates than could be found in published sources: 2.5-3 times higher than calculated for 100 ps, ca. 1.25-fold higher than experimental evaluation for nano- and femtosecond impact. We assume that the difference may be due to a change in the actual absorptivity of the target upon repeated impact, the spatial shape of the beam (homogeneous or Gaussian), and the experimental methods used (target temperature or through the heat flux). The results obtained are highly novel and important for correct modeling of thermal coupling and adequate transition from laboratory to real systems using repetitively pulsed picosecond impacts.
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