激光器
高次谐波产生
光学
路径(计算)
方案(数学)
谐波分析
物理
谐波
计算机科学
电子工程
工程类
声学
数学
数学分析
程序设计语言
作者
Peter Šušnjar,Alexander Demidovich,G. Kurdi,Paolo Cinquegrana,I. Nikolov,Paolo Sigalotti,M. Danailov
标识
DOI:10.1364/cleo_at.2024.jw2a.217
摘要
Ultrashort pulses in the deep-UV region around 200 nm have important applications in laser spectroscopy and Free-Electron laser technology [1,2]. Such pulses can be obtained using Ti:Sapphire laser followed by a fourth harmonic generation (FHG). In this case due to phase matching limitations of the available nonlinear crystals the fourth harmonic (FH) can only be generated in a three-step setup starting with second harmonic generation (SHG), followed by third harmonic generation (THG) realized by sum frequency mixing (SF) of SH and fundamental pulses, and then a final FHG stage based on sum frequency mixing of third harmonic (TH) and fundamental pulses.
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