使用视频速率频率分辨光门系统的实时飞秒光脉冲测量

J. Garduno, D. Reid
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摘要

二次谐波频率分辨光门控(SHG-FROG)已经成为测量锁模飞秒激光器产生的超快光脉冲的幅度和相位的一种常用和可靠的技术。通常,SHG-FROG测量是在几秒到几分钟的时间内进行的,通过使用慢速扫描延迟线耦合到单镜头光谱仪和其他技术来加快采集速率。在这项工作中,我们展示了一个实用的系统,该系统基于同步快速扫描振镜和延迟线,这样SHG-FROG轨迹就可以直接在视频监视器上看到,并且可以使用与个人计算机接口的图像采集板进行采集和处理。与其他快速获取SHGFROG轨迹的方法相比,该系统提供了比其他机械扫描实现更直接的输出,并且由于能够控制测量轨迹的时间宽度,因此比单次射击设备更具通用性。该系统如图1所示,包括一个色散平衡扫描干涉仪,该干涉仪包括镀银中空后向反射器和一个薄分光器(RI, R2和BS)。其中一个反向反射器是静态的,另一个使用压电平移器以大约40赫兹的频率扫描。调整后向反射镜。因此,从干涉仪中产生的脉冲是两个平行但非共线的光束,这些光束集中入射到凹面金镜(MZ)上。金反射镜折叠后的焦点路径使用了来自平面金反射镜的近正入射反射,该反射镜引导光束通过弯曲反射镜进入I型相位匹配的200mm厚的硼酸钡(BBO)晶体,在那里它们以一个小的交叉角结合。——人工智能
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Real time femtosecond optical pulse measurement using a video-rate frequency-resolved-optical-gating system
Second-harmonic frequency resolved optical gating (SHG-FROG) has become a common and reliable technique for the measurement of the amplitude and phase of ultrafast optical pulses of the kind typically produced by mode-locked femtosecond laser. Commonly SHG-FROG measurement is carried out over a period of several seconds to many minutes by using a slowly scanning delay-line coupled to a single-shot spectrometer and other techniques to speed up the acquisition rate.'.' In this work we demonstrate a practical system based on synchronising a fast scanning galvanometer mirror and delay line in such a way that the SHG-FROG trace is viewed directly on a video-monitor and can be acquired and processed using in image acquisition board interfaced to a personal computer. Compared to alternative approaches for rapidly-acquiring a SHGFROG trace, the system provides a more direct output than other mechanically-scanning implementations and is more versatile than a single-shot device because of the ability to control the temporal width of the measured trace. The system is presented in Figure 1 and comprises a dispersion-balanced scanning interferometer that includes silver-coated hollow retro-reflectors and a thin beamsplitter (RI, R2 and BS). One of the retro-reflectors is static and the other is scanned at around 40 Hz using a piezo-electric translalor. The retro-reflectors are adjusted.so the pulses emerge from the interferometer as two parallel but non-collinear beams and these are incident centrally on a concave gold mirror (MZ). The focal path after the gold mirror is folded using a near-normal incidence reflection from a plane gold mirror which steers the beams past the curved mirror and into a Type I phasematched 200pmthick beta-barium borate (BBO) crystal where they combine with a small crossing angle. - aI
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