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Interaction of extreme ultraviolet laser radiation with solid surface: ablation, desorption, nanostructuring

机译:极紫外激光辐射与固体表面的相互作用:消融,解吸,纳米结构

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The area, where interaction of focused XUV laser radiation with solid surface takes place, can be divided according to local fluency into desorption region (if fluency is larger than zero and smaller than ablation threshold) and ablation region (if fluency is equal or larger than this threshold). It turned out that a direct nanostructuring (e.g. imprinting diffraction pattern created on edges of windows of proximity standing grid) is possible in the desorption region only. While for femtosecond pulses the particle (atom/molecule) removal-efficiency η in the desorption region is very small (η< 10%), and hence, it can be easily distinguished from the ablation region with η ~ 100%, for nanosecond pulses in desorption region this η rises at easily ablated materials from 0% at the periphery up to ~ 90% at the ablation contour and, therefore, the boundary between these two regions can be found with the help of nanostructuring only. This rise of removal efficiency could be explained by gradually increased penetration depth (due to gradually removed material) during laser pulse. This is a warning against blind using crater shape for fluency mapping in the case of long laser pulses. On the other hand it is a motivation to study an ablation plum (or ablation jet) and to create a knowledge bank to be used at future numerical modeling of this process.
机译:聚焦的XUV激光辐射与固体表面发生相互作用的区域可以根据局部流利度分为解吸区(如果流利度大于零且小于消融阈值)和消融区(如果流利度等于或大于)。此阈值)。事实证明,仅在解吸区域中可能进行直接的纳米结构化(例如,在邻近的直立网格的窗口的边缘上产生的压印衍射图样)。对于飞秒脉冲,解吸区域中的粒子(原子/分子)去除效率η非常小(η<10%),因此,对于纳秒脉冲,可以轻松地将其与η〜100%的消融区域区分开。在解吸区,该η在易烧蚀材料处从周围的0%上升到烧蚀轮廓处的〜90%,因此,这两个区域之间的边界只能借助纳米结构来找到。去除效率的这种提高可以通过在激光脉冲期间逐渐增加的穿透深度(由于逐渐去除的材料)来解释。在长脉冲激光的情况下,这是警告不要盲目地使用坑状形状进行流利性映射。另一方面,这是研究消融李子(或消融射流)并创建知识库以用于该过程的未来数值建模的动机。

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