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首页> 外文期刊>Journal of Modern Optics >Coherence conversion for optimized resolution in optical measurements - example of femtosecond time resolution using the transverse coherence of 100-picosecond X-rays
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Coherence conversion for optimized resolution in optical measurements - example of femtosecond time resolution using the transverse coherence of 100-picosecond X-rays

机译:相干转换以优化光学测量的分辨率-使用100皮秒X射线的横向相干的飞秒时间分辨率示例

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摘要

A way is proposed to obtain a femtosecond time resolution over a picosecond range in laser-pump, X-ray probe spectroscopic measurements where the light source and the detector are much slower than that. It is based on a phase-space transformation from the time/bandwidth to the spatial/wavenumber domain to match the coherence properties of synchrotron radiation to the requirements of femtosecond experiments. In a first step, the geometry of the laser incidence maps time, t, of laser-induced femtosecond dynamics to a spatial coordinate, x. Then, a far-field X-ray diffraction pattern, i.e. the optical Fourier transform, is obtained from the laser-induced modifications of the sample properties, including shifts of X-ray absorption edges and changes in crystallographic unit-cell form factors. Whereas the first step is similar to previously used schemes for femtosecond time resolution, the second one is substantially different with specific advantages discussed in the text. Key to this technique is that the modulus of the Fourier transform is invariant with respect to translations along x, which are due to the correlation. It can, therefore, be acquired in a simple intensity measurement with a slow detector. The phase, which does vary strongly with , is missing in the intensity data, but can be recovered through a heterodyning technique. Data from a demonstration experiment are presented. The same concept can be used to obtain attosecond time resolution with an X-ray free-electron laser.
机译:提出了一种在激光泵,X射线探针光谱测量中获得皮秒范围内飞秒时间分辨率的方法,其中光源和检测器要慢得多。它基于从时间/带宽到空间/波数域的相空间转换,以使同步加速器辐射的相干特性与飞秒实验的要求相匹配。在第一步中,激光入射的几何形状将激光诱导的飞秒动力学的时间t映射到空间坐标x。然后,通过激光诱导的样品特性的改变,包括X射线吸收边缘的移动和晶体学晶胞形状因子的变化,获得了远场X射线衍射图,即光学傅里叶变换。第一步类似于先前使用的飞秒时间分辨率方案,而第二步与本文讨论的特定优势大不相同。该技术的关键在于,傅里叶变换的模数相对于平移是不变的 沿x,这是由于 相关性。因此,可以使用慢速检测器通过简单的强度测量来获取它。该阶段与 的确存在很大差异在强度数据中,但可以通过外差技术恢复。展示了来自示范实验的数据。可以使用相同的概念通​​过X射线自由电子激光器获得亚秒级的时间分辨率。

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