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首页> 外文期刊>Physical review letters >Ultrafast Adsorbate Excitation Probed with Subpicosecond-Resolution X-Ray Absorption Spectroscopy
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Ultrafast Adsorbate Excitation Probed with Subpicosecond-Resolution X-Ray Absorption Spectroscopy

机译:超速率吸附探测亚磷二秒分辨率X射线吸收光谱法探测

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摘要

We use a pump-probe scheme to measure the time evolution of the C K-edge x-ray absorption spectrum from CO/Ru(0001) after excitation by an ultrashort high-intensity optical laser pulse. Because of the short duration of the x-ray probe pulse and precise control of the pulse delay, the excitation-induced dynamics during the first picosecond after the pump can be resolved with unprecedented time resolution. By comparing with density functional theory spectrum calculations, we find high excitation of the internal stretch and frustrated rotation modes occurring within 200 fs of laser excitation, as well as thermalization of the system in the picosecond regime. The similar to 100 fs initial excitation of these CO vibrational modes is not readily rationalized by traditional theories of nonadiabatic coupling of adsorbates to metal surfaces, e.g., electronic frictions based on first order electron-phonon coupling or transient population of adsorbate resonances. We suggest that coupling of the adsorbate to nonthermalized electron-hole pairs is responsible for the ultrafast initial excitation of the modes.
机译:我们使用泵探针方案来测量通过超短高强度光激光脉冲激发后的Co / Ru(0001)的C k边X射线吸收光谱的时间演变。由于X射线探测脉冲的短暂持续时间和脉冲延迟的精确控制,可以通过前所未有的时间分辨率解决泵之后的第一皮秒内的激励引起的动态。通过与密度函数理论谱计算进行比较,我们在激光激发的200 fs内发生的内部拉伸和沮丧的旋转模式的高励磁,以及在皮秒内的系统的热化。与这些CO振动模式的类似100 fs初始激发不容易通过传统的吸附与金属表面的非等压偶联的理论,例如基于第一阶电子 - 声子耦合或吸附血管共振的瞬态群的电子摩擦的理论。我们认为吸附物与非热化电子 - 孔对的耦合负责超快的初始激发模式。

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  • 来源
    《Physical review letters》 |2021年第1期|016802.1-016802.6|共6页
  • 作者单位

    SLAC Natl Accelerator Lab SUNCAT Ctr Interface Sci & Catalysis 2575 Sand Hill Rd Menlo Pk CA 94025 USA;

    Stockholm Univ Alballova Univ Ctr Dept Phys SE-10691 Stockholm Sweden;

    Stockholm Univ Alballova Univ Ctr Dept Phys SE-10691 Stockholm Sweden;

    Stockholm Univ Alballova Univ Ctr Dept Phys SE-10691 Stockholm Sweden;

    SLAC Natl Accelerator Lab 2575 Sand Hill Rd Menlo Pk CA 94025 USA;

    Chapman Univ Schmid Coll Sci & Technol Orange CA 92866 USA;

    Stockholm Univ Alballova Univ Ctr Dept Phys SE-10691 Stockholm Sweden;

    CNR IOM SS 14 Km 163 I-34149 Trieste Italy;

    Elettra Sincrotrone Trieste FERM SS 14 Km 163-5 I-34149 Trieste Italy;

    Elettra Sincrotrone Trieste FERM SS 14 Km 163-5 I-34149 Trieste Italy;

    Elettra Sincrotrone Trieste FERM SS 14 Km 163-5 I-34149 Trieste Italy;

    Elettra Sincrotrone Trieste FERM SS 14 Km 163-5 I-34149 Trieste Italy;

    Elettra Sincrotrone Trieste FERM SS 14 Km 163-5 I-34149 Trieste Italy;

    Elettra Sincrotrone Trieste FERM SS 14 Km 163-5 I-34149 Trieste Italy;

    Elettra Sincrotrone Trieste FERM SS 14 Km 163-5 I-34149 Trieste Italy;

    DESY Photon Sci Notkestr 85 D-22607 Hamburg Germany;

    Stockholm Univ Alballova Univ Ctr Dept Phys SE-10691 Stockholm Sweden;

    Stockholm Univ Alballova Univ Ctr Dept Phys SE-10691 Stockholm Sweden;

    Stockholm Univ Alballova Univ Ctr Dept Phys SE-10691 Stockholm Sweden|SLAC Natl Accelerator Lab 2575 Sand Hill Rd Menlo Pk CA 94025 USA;

    Stockholm Univ Alballova Univ Ctr Dept Phys SE-10691 Stockholm Sweden;

    DESY Photon Sci Notkestr 85 D-22607 Hamburg Germany;

    CNR IOM SS 14 Km 163 I-34149 Trieste Italy|Univ Trieste Phys Dept Via Valerio 2 I-34127 Trieste Italy;

    SLAC Natl Accelerator Lab 2575 Sand Hill Rd Menlo Pk CA 94025 USA|Stanford Univ Dept Appl Phys Stanford CA 94305 USA;

    SLAC Natl Accelerator Lab SUNCAT Ctr Interface Sci & Catalysis 2575 Sand Hill Rd Menlo Pk CA 94025 USA;

    SLAC Natl Accelerator Lab SUNCAT Ctr Interface Sci & Catalysis 2575 Sand Hill Rd Menlo Pk CA 94025 USA;

    SLAC Natl Accelerator Lab SUNCAT Ctr Interface Sci & Catalysis 2575 Sand Hill Rd Menlo Pk CA 94025 USA;

    Stockholm Univ Alballova Univ Ctr Dept Phys SE-10691 Stockholm Sweden;

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