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    Reduction of electron-phonon coupling in warm dense iron

    A. Fernandez-Pañella1,*, T. Ogitsu1, K. Engelhorn2, A. A. Correa1, B. Barbrel3, S. Hamel1, D. G. Prendergast4, D. Pemmaraju4, M. A. Beckwith1 et al.

    L. J. Bae5, J. W. Lee5, B. I. Cho5, P. A. Heimann6, R. W. Falcone3, and Y. Ping1

    • 1Lawrence Livermore National Laboratory, Livermore, California 94550, USA
    • 2Advanced Light Source, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
    • 3Department of Physics, UC Berkeley, Berkeley, California 94720, USA
    • 4The Molecular Foundry, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
    • 5Department of Physics and Photon Science, Gwangju Institute of Science and Technology, Gwangju, Korea
    • 6Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA

    • *Corresponding author: ping2@llnl.gov

    Phys. Rev. B 101, 184309 – Published 28 May, 2020

    DOI: https://doi.org/10.1103/PhysRevB.101.184309

    Abstract

    The electron-ion relaxation dynamics in warm dense iron were investigated by time-resolved x-ray absorption near-edge spectroscopy (XANES). A novel analysis, combining ab initio density functional theory (DFT) and two temperature model (TTM) simulations, was developed to calculate the x-ray absorption spectra as a function of delay time. Here we present experimental evidence of changes at the XAS L3 edge of iron that are consistent with the reduction of the electron-phonon coupling under warm dense matter conditions. The experimental results are in agreement with the model that takes both the electron (Te) and the ion temperature (Ti) dependence of the thermophysical properties into consideration, while models where either constant electron-phonon coupling factor (G) or only Te-dependent G are used do not agree with the observed relaxation dynamics of iron.

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