Zhang Simin, Menoni Carmen, Gruzdev Vitaly, Chowdhury Enam
Department of Material Science and Engineering, The Ohio State University, Columbus, OH 43210, USA.
Electrical and Computer Engineering Department, Colorado State University, Fort Collins, CO 80523, USA.
Nanomaterials (Basel). 2022 Apr 8;12(8):1259. doi: 10.3390/nano12081259.
The chirped pulse amplification technique has enabled the generation of pulses of a few femtosecond duration with peak powers multi-Tera and Peta-Watt in the near infrared. Its implementation to realize even shorter pulse duration, higher energy, and higher repetition rate laser systems relies on overcoming the limitations imposed by laser damage of critical components. In particular, the laser damage of coatings in the amplifiers and in post-compression optics have become a bottleneck. The robustness of optical coatings is typically evaluated numerically through steady-state simulations of electric field enhancement in multilayer stacks. However, this approach cannot capture crucial characteristics of femtosecond laser induced damage (LID), as it only considers the geometry of the multilayer stack and the optical properties of the materials composing the stack. This approach neglects that in the interaction of an ultrashort pulse and the materials there is plasma generation and associated material modifications. Here, we present a numerical approach to estimate the LID threshold of dielectric multilayer coatings based on strong field electronic dynamics. In this dynamic scheme, the electric field propagation, photoionization, impact ionization, and electron heating are incorporated through a finite-difference time-domain algorithm. We applied our method to simulate the LID threshold of bulk fused silica, and of multilayer dielectric mirrors and gratings. The results are then compared with experimental measurements. The salient aspects of our model, such as the implementation of the Keldysh photoionization model, the impact ionization model, the electron collision model for 'low'-temperature, dense plasma, and the LID threshold criterion for few-cycle pulses are discussed.
啁啾脉冲放大技术已能够产生持续时间为几飞秒、峰值功率在近红外波段达到多太瓦和拍瓦级的脉冲。要实现更短脉冲持续时间、更高能量和更高重复频率的激光系统,其实施依赖于克服关键部件激光损伤所带来的限制。特别是,放大器和后压缩光学元件中涂层的激光损伤已成为一个瓶颈。光学涂层的稳健性通常通过多层膜堆中电场增强的稳态模拟进行数值评估。然而,这种方法无法捕捉飞秒激光诱导损伤(LID)的关键特性,因为它仅考虑多层膜堆的几何结构以及构成膜堆的材料的光学性质。这种方法忽略了在超短脉冲与材料的相互作用中会产生等离子体以及相关的材料改性。在此,我们提出一种基于强场电子动力学来估计介电多层涂层LID阈值的数值方法。在这种动态方案中,通过时域有限差分算法纳入了电场传播、光电离、碰撞电离和电子加热。我们应用我们的方法来模拟块状熔融石英以及多层介质镜和光栅的LID阈值。然后将结果与实验测量值进行比较。讨论了我们模型的显著方面,例如凯尔迪什光电离模型、碰撞电离模型、“低温”、高密度等离子体的电子碰撞模型以及少周期脉冲的LID阈值准则的实施。