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在倾斜入射时,通过强场中红外激光与锗固体相互作用在锗中形成激光诱导周期性表面结构。

Laser induced periodic surface structure formation in germanium by strong field mid IR laser solid interaction at oblique incidence.

作者信息

Austin Drake R, Kafka Kyle R P, Trendafilov Simeon, Shvets Gennady, Li Hui, Yi Allen Y, Szafruga Urszula B, Wang Zhou, Lai Yu Hang, Blaga Cosmin I, DiMauro Louis F, Chowdhury Enam A

出版信息

Opt Express. 2015 Jul 27;23(15):19522-34. doi: 10.1364/OE.23.019522.

Abstract

Laser induced periodic surface structures (LIPSS or ripples) were generated on single crystal germanium after irradiation with multiple 3 µm femtosecond laser pulses at a 45° angle of incidence. High and low spatial frequency LIPSS (HSFL and LSFL, respectively) were observed for both s- and p-polarized light. The measured LSFL period for p-polarized light was consistent with the currently established LIPSS origination model of coupling between surface plasmon polaritons (SPP) and the incident laser pulses. A vector model of SPP coupling is introduced to explain the formation of s-polarized LSFL away from the center of the damage spot. Additionally, a new method is proposed to determine the SPP propagation length from the decay in ripple depth. This is used along with the measured LSFL period to estimate the average electron density and Drude collision time of the laser-excited surface. Finally, full-wave electromagnetic simulations are used to corroborate these results while simultaneously offering insight into the nature of LSFL formation.

摘要

在用多个3微米飞秒激光脉冲以45°入射角照射后,在单晶锗上产生了激光诱导的周期性表面结构(LIPSS或波纹)。对于s偏振光和p偏振光,均观察到了高空间频率和低空间频率的LIPSS(分别为HSFL和LSFL)。p偏振光的测量LSFL周期与当前已确立的表面等离激元极化激元(SPP)与入射激光脉冲之间耦合的LIPSS起源模型一致。引入了SPP耦合矢量模型来解释远离损伤点中心的s偏振LSFL的形成。此外,还提出了一种从波纹深度衰减确定SPP传播长度的新方法。这与测量的LSFL周期一起用于估计激光激发表面的平均电子密度和德鲁德碰撞时间。最后,使用全波电磁模拟来证实这些结果,同时深入了解LSFL形成的本质。

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