Non-isotropic Atomic Motion in Warm Dense Carbon

ORAL

Abstract

X-ray Free Electron Laser (XFEL) radiation can transform carbon into a warm dense matter state. Two X-ray pulses were used; the first as pump to reach the warm dense matter state and the second as probe performing X-ray diffraction. The experiment was performed at the SACLA XFEL facility at the beamline 3 experimental hutch 5. The samples were polycrystalline diamond. The pump and probe photon energies were 7 and 10.5 keV, respectively, and the delay between the X-ray pulses was varied from 0 to 286 fs. To provide a range of energy densities, the X-ray focus was adjusted between 150 nm and 1 μm. The (111), (220) and (311) diffraction peaks were observed. The intensity of each diffraction peak decreased with time indicating a disordering of the crystal lattice. From a Debye-Waller analysis, the root-mean-square (rms) atomic displacement perpendicular to particular lattice planes are calculated. At higher fluences, the rms atomic displacement perpendicular to the (111) planes is significantly larger than that perpendicular to the (220) or (311) planes. By accepting two successive XFEL pulses at a time delay of 33 ms, graphite (002) diffraction was observed beginning at a threshold dose of 1.5 eV/atom. The experimental results will be compared with calculations using a hybrid model based on tight-binding molecular dynamics.

Presenters

  • Philip Heimann

    • SLAC - Natl Accelerator Lab

Authors

  • Philip Heimann

    • SLAC - Natl Accelerator Lab
  • Nicholas J Hartley

    • SLAC - Natl Accelerator Lab
  • Ichiro Inoue

    • RIKEN SPring-8 Center, 1-1-1 Kouto, Sayo, Hyogo 679-5148, Japan
  • Andre F Antoine

    • University of Michigan
  • Fabien Dorchies

    • Universit´e de Bordeaux, CNRS, CEA, Centre Lasers Intenses et Applications, UMR 5107, F-33400 Talence, France
  • Roger Falcone

    • University of California, Berkeley
  • Jérôme Gaudin

    • Universit´e de Bordeaux, CNRS, CEA, Centre Lasers Intenses et Applications, UMR 5107, F-33400 Talence, France
  • Hauke Hoeppner

    • European XFEL GmbH, Holzkoppel 4, 22869 Schenefeld, Germany
  • Yuichi Inubushi

    • RIKEN SPring-8 Center, 1-1-1 Kouto, Sayo, Hyogo 679-5148, Japan
  • Hae Ja Lee

    • SLAC National Accelerator Laboratory
    • Linac Coherent Light Source, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California, 94025, USA
  • Vladimir Lipp

    • Deutsches Elektronen-Synchrotron, Notkestr. 85, 22607 Hamburg, Germany
  • Paloma Martinez

    • Universit´e de Bordeaux, CNRS, CEA, Centre Lasers Intenses et Applications, UMR 5107, F-33400 Talence, France
  • Nikita Medvedev

    • Institute of Physics, Czech Academy of Sciences
  • Franz Tavella

    • Linac Coherent Light Source, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California, 94025, USA
  • Victor Tkachenko

    • Deutsches Elektronen-Synchrotron, Notkestr. 85, 22607 Hamburg, Germany
  • Sven Toleikis

    • Deutsches Elektronen-Synchrotron, Notkestr. 85, 22607 Hamburg, Germany
  • Makina Yabashi

    • RIKEN SPring-8 Center, 1-1-1 Kouto, Sayo, Hyogo 679-5148, Japan
  • Toshinori Yabuuchi

    • Japan Synchrotron Radiation Institute (JSRI)
  • Jumpei Yamada

    • RIKEN SPring-8 Center, 1-1-1 Kouto, Sayo, Hyogo 679-5148, Japan
  • Beata Ziaja-Motyka

    • Deutsches Elektronen-Synchrotron, Notkestr. 85, 22607 Hamburg, Germany