单飞秒光脉冲的相位畸变跟踪

V. Kabelka, A. Masalov, S. Nikitin, H. Milchberg
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引用次数: 0

摘要

首次实现了一种基于非共线二次谐波产生自相关器的频率示踪器(FT),可在不使用光谱仪器的情况下对单飞秒光脉冲进行二维时频成像[1]。通过测量啁啾脉冲放大Ti:蓝宝石激光系统产生的飞秒脉冲的瞬时频率,进行了频率示踪的实验测试。在正常运行中,系统能够产生高达1.5兆焦耳能量的脉冲和大约90秒持续时间的FWHM。采集了不同压缩光栅间距下脉冲的频率迹线。用一个简单的模型对线性啁啾和脉冲持续时间的实验数据进行了检验,其中高斯脉冲由于在压缩器中通过一对衍射光栅之间的色散路径传播而形状发生了变化。当光栅分离偏离其最优值时,输出脉冲的光谱分量会发生二次相移(以频率为单位)。啁啾和脉冲持续时间对光栅分离的影响与系统输出色散的估计一致。配准后的图像不仅显示出脉冲的线性啁啾(测量结果明确),而且显示出四阶相位畸变(三次啁啾)。我们通过数值计算证明,频率示踪器产生的图像具有简单的直观意义:频率示踪是由二维图像的极大值形成的,不需要任何迭代检索算法来可视化相位畸变[2]。计算结果表明,该二次谐波示踪器可以测量飞秒光脉冲的偶阶相位畸变:啁啾、四阶等。这些畸变包括对称脉冲的相位自调制(克尔非线性贡献)。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Tracing the Phase Distortion of a Single Femtosecond Light Pulse
A frequency tracer (FT) based on noncollinear second harmonic generation autocorrelator for two-dimensional time-frequency imaging of a single femtosecond light pulse without using a spectral apparatus [1] had implemented for a first time. An experimental test of frequency tracer has been performed by measuring the instantaneous frequency of femtosecond pulses produced by a chirped pulse amplification Ti:sapphire laser system. In a normal operation the system is able to produce pulses up to 1.5 mJ energy and about 90 fs duration FWHM. The frequency traces were collected for pulses at different compressor grating separations. Experimental data on the linear chirp and pulse duration have been checked against a simple model, where the shape of the gausian pulse changes due to propagation through a dispersive path between pair of diffraction grating in a compressor. Detuning of the grating separation from its optimal value results in quadratic (in terms of frequency) phase shift of spectral components of output pulse. The data on chirp and pulse duration versus grating separation are in a good agreement with the estimations of dispersions at the system output. The registered images shown not only linear chirp of pulses (which was measured unambiguously) but also the fourth order phase distortion (cubic chirp). We prove by numerical calculations that images produced by the frequency tracer have simple intuitive meaning: the frequency trace is formed by maxima of two-dimensional image and does not require any iterative retrieval algorithm for visualising the phase distortions [2]. The calculations show that the second-harmonic frequency tracer allows to measure the even-order phase distortions of femtosecond light pulses: chirp, fourth-order, etc. These distortions include the phase self-modulation (Kerr-nonlinear contribution) of symmetric pulse.
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