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Femtosecond electronic response of atoms to ultra-intense X-rays

机译:飞秒原子对超强X射线的电子响应

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摘要

An era of exploring the interactions of high-intensity, hard X-rays with matter has begun with the start-up of a hard-X-ray free-electron laser, the Linac Coherent Light Source (LCLS). Understanding how electrons in matter respond to ultra-intense X-ray radiation is essential for all applications. Here we reveal the nature of the electronic response in a free atom to unprecedented high-intensity, short-wavelength, high-fluence radiation (respectively 10~(18) W cm~(-2),1.5-0.6 nm, ~10~5 X-ray photons per A~2). At this fluence, the neon target inevitably changes during the course of a single femtosecond-duration X-ray pulse-by sequentially ejecting electrons-to produce fully-stripped neon through absorption of six photons. Rapid photoejection of inner-shell electrons produces 'hollow' atoms and an intensity-induced X-ray transparency. Such transparency, due to the presence of inner-shell vacancies, can be induced in all atomic, molecular and condensed matter systems at high intensity. Quantitative comparison with theory allows us to extract LCLS fluence and pulse duration. Our successful modelling of X-ray/atom interactions using a straightforward rate equation approach augurs favourably for extension to complex systems.
机译:探索高强度硬X射线与物质相互作用的时代已经开始于硬X射线自由电子激光器,直线加速器相干光源(LCLS)的启动。了解物质中的电子如何响应超强X射线辐射对于所有应用至关重要。在这里,我们揭示了游离原子对空前的高强度,短波长,高通量辐射(分别为10〜(18)W cm〜(-2),1.5-0.6 nm,〜10〜每个A〜2有5个X射线光子)。在这种能量密度下,霓虹灯目标在单个飞秒持续时间的X射线脉冲过程中会不可避免地发生变化,方法是依次喷射电子,以吸收六个光子来产生完全剥离的霓虹灯。内壳电子的快速光喷射产生“空心”原子和强度感应的X射线透明性。由于存在内壳空位,这种透明性可以在所有原子,分子和凝聚态系统中以高强度诱导。与理论的定量比较使我们能够提取LCLS积分通量和脉冲持续时间。我们使用简单的速率方程式方法成功地对X射线/原子相互作用进行建模,预示着扩展到复杂系统的前景。

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  • 来源
    《Nature》 |2010年第7302期|P.56-61ⅲ|共7页
  • 作者单位

    Argonne National Laboratory, Argonne, Illinois 60439, USA;

    Argonne National Laboratory, Argonne, Illinois 60439, USA;

    Argonne National Laboratory, Argonne, Illinois 60439, USA;

    Argonne National Laboratory, Argonne, Illinois 60439, USA;

    Argonne National Laboratory, Argonne, Illinois 60439, USA;

    Argonne National Laboratory, Argonne, Illinois 60439, USA;

    rnArgonne National Laboratory, Argonne, Illinois 60439, USA The University of Chicago, Chicago, Illinois 60637, USA;

    rnArgonne National Laboratory, Argonne, Illinois 60439, USA;

    rnLawrence Livermore National Laboratory, Livermore, California 94551, USA;

    rnThe Ohio State University, Columbus, Ohio 43210, USA;

    rnThe Ohio State University, Columbus, Ohio 43210, USA;

    rnThe Ohio State University, Columbus, Ohio 43210, USA;

    rnWestern Michigan University, Kalamazoo, Michigan 49008, USA;

    rnWestern Michigan University, Kalamazoo, Michigan 49008, USA;

    rnWestern Michigan University, Kalamazoo, Michigan 49008, USA Western Michigan University, Kalamazoo, Michigan 49008, USA;

    rnPULSE Institute, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA;

    rnPULSE Institute, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA;

    rnPULSE Institute, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA;

    rnPULSE Institute, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA;

    rnPULSE Institute, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA;

    rnLinac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA;

    Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA;

    Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA;

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  • 正文语种 eng
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  • 入库时间 2022-08-18 02:55:09

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