Femtosecond single-pass optical parametric generator (OPG) for 1.38-1.56 μm with 35 MHz repetition rate

T. Siidmeyer, J. A. Au, R. Paschotta, U. Keller, G. R. Smith, G. Ross, D. Hanna
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Abstract

Optical parametric generation (OPG) in a single pass through a χ(2) nonlinear crystal is a simple way to generate ultrashort pulses which are tunable in a broad wavelength range. In contrast to an ultrafast optical parametric oscillator, OPG does not require an oscillator cavity which is synchronized to the laser. However, the required pump intensities are much higher. For this reason, so far OPG experiments with ultrashort pulses have always required amplified pump sources, e.g. based on a mode-locked oscillator and a high-gain amplifier operated at a repetition rate of typically far below 1 MHz [1, 2]. Such pump sources lead to quite complex systems, and low repetition rates very much limit the obtainable average output power. Recent progress on high-power passively mode-locked all-solid-state lasers has enabled us to pump a parametric generator directly with a mode-locked laser, not using any amplifier system. In this way we obtained up to 0.5 W of average power in femtosecond pulses at 35 MHz repetition rate in the wavelength range of 1.38-1.56 μm using a periodically poled LiNbO3 (PPLN) crystal. The corresponding range of the idler is 3.03-4.06 μm.
1.38 ~ 1.56 μm的飞秒单通光参量发生器(OPG), 35 MHz重复频率
单次通过χ(2)非线性晶体的光参数生成(OPG)是一种产生超短脉冲的简单方法,该脉冲在宽波长范围内可调谐。与超快光学参量振荡器相比,OPG不需要与激光同步的振荡腔。然而,所需的泵浦强度要高得多。因此,到目前为止,使用超短脉冲的OPG实验总是需要放大泵浦源,例如基于锁模振荡器和高增益放大器,其重复频率通常远低于1 MHz[1,2]。这种泵源导致相当复杂的系统,低重复率极大地限制了可获得的平均输出功率。高功率被动锁模全固态激光器的最新进展使我们能够直接使用锁模激光器泵浦参数发生器,而不使用任何放大器系统。利用周期性极化的PPLN晶体,在1.38 ~ 1.56 μm波长范围内获得了35 MHz重复频率的飞秒脉冲平均功率高达0.5 W。惰轮对应的范围为3.03 ~ 4.06 μm。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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