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Establishing nonthermal regimes in pump-probe electron relaxation dynamics

机译:在泵探针电子松弛动力学中建立非热政策

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Time- and angle-resolved photoemission spectroscopy (TR-ARPES) accesses the electronic structure of solids under optical excitation, and is a powerful technique for studying the coupling between electrons and collective modes. One approach to infer electron-boson coupling is through the relaxation dynamics of optically excited electrons, and the characteristic timescales of energy redistribution. A common description of electron relaxation dynamics is through the effective electronic temperature. Such a description requires that thermodynamic quantities are well-defined, an assumption that is generally violated at early delays. Additionally, precise estimation of the nonthermal window-within which effective temperature models may not be applied-is challenging. We perform TR-ARPES on graphite and show that Boltzmann rate equations can be used to calculate the time-dependent electronic occupation function f(∈, t), and reproduce experimental features given by nonthermal electron occupation. Using this model, we define a quantitative measure of nonthermal electron occupation and use it to define distinct phases of electron relaxation in the fluence-delay phase space. More generally, this approach can be used to inform the nonthermal-to-thermal crossover in pump-probe experiments.
机译:时间和角度分辨的光曝光光谱(TR-ARPES)在光学激发下访问固体的电子结构,是研究电子和集体模式之间的耦合的强大技术。推断电子 - 玻色子耦合的一种方法是通过光学激发电子的松弛动力学,以及能量再分配的特征时间表。电子松弛动力学的常见描述是通过有效的电子温度。这种描述要求热力学量是良好的定义,假设通常在早期延迟处侵犯。另外,精确地估计了非热窗口 - 在该有效温度模型中可能无法应用 - 是具有挑战性的。我们在石墨上执行TR-ARPES,并表明Boltzmann速率方程可用于计算时间依赖的电子占用功能F(∈,T),并通过非热电子占用给出的实验特征。使用该模型,我们定义了非热电子占用的定量测量,并使用它来定义流量延迟相空间中的电子松弛的不同阶段。更一般地,这种方法可用于通知泵探针实验中的非热转换。

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  • 来源
    《Physical review.B.Condensed matter and materials physics》 |2020年第18期|184307.1-184307.16|共16页
  • 作者单位

    Quantum Matter Institute University of British Columbia Vancouver BC Canada V6T 1Z4 Department of Physics and Astronomy University of British Columbia Vancouver BC Canada V6T 1Z1;

    Quantum Matter Institute University of British Columbia Vancouver BC Canada V6T 1Z4 Department of Physics and Astronomy University of British Columbia Vancouver BC Canada V6T 1Z1 Centre Energie Materiaux Telecommunications Institut National de la Recherche Scientifique Varennes Quebec Canada J3X 1S2;

    Quantum Matter Institute University of British Columbia Vancouver BC Canada V6T 1Z4 Department of Physics and Astronomy University of British Columbia Vancouver BC Canada V6T 1Z1;

    Quantum Matter Institute University of British Columbia Vancouver BC Canada V6T 1Z4 Department of Physics and Astronomy University of British Columbia Vancouver BC Canada V6T 1Z1 Max Planck Institute for Chemical Physics of Solids 01187 Dresden Germany;

    Quantum Matter Institute University of British Columbia Vancouver BC Canada V6T 1Z4 Department of Physics and Astronomy University of British Columbia Vancouver BC Canada V6T 1Z1;

    Quantum Matter Institute University of British Columbia Vancouver BC Canada V6T 1Z4 Department of Physics and Astronomy University of British Columbia Vancouver BC Canada V6T 1Z1;

    Quantum Matter Institute University of British Columbia Vancouver BC Canada V6T 1Z4 Department of Physics and Astronomy University of British Columbia Vancouver BC Canada V6T 1Z1;

    Quantum Matter Institute University of British Columbia Vancouver BC Canada V6T 1Z4 Department of Physics and Astronomy University of British Columbia Vancouver BC Canada V6T 1Z1;

    Department of Physics North Carolina State University Raleigh North Carolina 27695 USA;

    Quantum Matter Institute University of British Columbia Vancouver BC Canada V6T 1Z4 Department of Physics and Astronomy University of British Columbia Vancouver BC Canada V6T 1Z1;

    Quantum Matter Institute University of British Columbia Vancouver BC Canada V6T 1Z4 Department of Physics and Astronomy University of British Columbia Vancouver BC Canada V6T 1Z1;

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