Second-order autocorrelation of XUV FEL pulses via time resolved two-photon single ionization of He.

Second-order autocorrelation of XUV FEL pulses via time resolved two-photon single ionization of He.
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DOI:
10.1364/oe.19.021698
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发表时间:
2011-10
期刊:
影响因子:
3.8
通讯作者:
R. Moshammer;T. Pfeifer;Artem Rudenko;Yuhai Jiang;L. Foucar;M. Kurka;K. Kühnel;C. Schröter;J. Ullrich;O. Herrwerth;Matthias F. Kling;XiaoJun Liu;K. Motomura;H. Fukuzawa;A. Yamada;K. Ueda;K. L. Ishikawa;K. Nagaya;H. Iwayama;A. Sugishima;Y. Mizoguchi;S. Yase;Makoto Yao;N. Saito;A. Belkacem;M. Nagasono;A. Higashiya;M. Yabashi;Tetsuya Ishikawa;H. Ohashi;H. Kimura;T. Togashi
R. Moshammer;T. Pfeifer;Artem Rudenko;Yuhai Jiang;L. Foucar;M. Kurka;K. Kühnel;C. Schröter;J. Ullrich;O. Herrwerth;Matthias F. Kling;XiaoJun Liu;K. Motomura;H. Fukuzawa;A. Yamada;K. Ueda;K. L. Ishikawa;K. Nagaya;H. Iwayama;A. Sugishima;Y. Mizoguchi;S. Yase;Makoto Yao;N. Saito;A. Belkacem;M. Nagasono;A. Higashiya;M. Yabashi;Tetsuya Ishikawa;H. Ohashi;H. Kimura;T. Togashi
中科院分区:
物理与天体物理2区
文献类型:
--
作者:
R. Moshammer;T. Pfeifer;Artem Rudenko;Yuhai Jiang;L. Foucar;M. Kurka;K. Kühnel;C. Schröter;J. Ullrich;O. Herrwerth;Matthias F. Kling;XiaoJun Liu;K. Motomura;H. Fukuzawa;A. Yamada;K. Ueda;K. L. Ishikawa;K. Nagaya;H. Iwayama;A. Sugishima;Y. Mizoguchi;S. Yase;Makoto Yao;N. Saito;A. Belkacem;M. Nagasono;A. Higashiya;M. Yabashi;Tetsuya Ishikawa;H. Ohashi;H. Kimura;T. Togashi

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利用分镜延迟级结合高分辨率反冲-离子动量谱(COLTRIMS)对20.45 eV双光子单电离He进行了时间和动量分辨探测,记录了来自Spring-8紧凑型SASE源(SCSS)的XUV自由电子激光脉冲的二阶自相关光谱。从自相关轨迹中,我们提取了相干时间为8±2 fs,平均脉冲持续时间为28±5 fs,比基于电子束长度测量的估计要短得多。部分相干模型内的模拟[Opt. Lett. 35, 3441(2010)]与实验结果一致,如果考虑到穿过FEL光束直径的脉冲前倾斜,将导致两个脉冲副本之间约6 fs的时间偏移。
Second-order autocorrelation spectra of XUV free-electron laser pulses from the Spring-8 Compact SASE Source (SCSS) have been recorded by time and momentum resolved detection of two-photon single ionization of He at 20.45 eV using a split-mirror delay-stage in combination with high-resolution recoil-ion momentum spectroscopy (COLTRIMS). From the autocorrelation trace we extract a coherence time of 8 ± 2 fs and a mean pulse duration of 28 ± 5 fs, much shorter than estimations based on electron bunch-length measurements. Simulations within the partial coherence model [Opt. Lett. 35, 3441 (2010)] are in agreement with experiment if a pulse-front tilt across the FEL beam diameter is taken into account that leads to a temporal shift of about 6 fs between both pulse replicas.