4.6 Article

X-ray absorption spectroscopy using a self-seeded soft X-ray free-electron laser

Journal

OPTICS EXPRESS
Volume 24, Issue 20, Pages 22469-22480

Publisher

OPTICAL SOC AMER
DOI: 10.1364/OE.24.022469

Keywords

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Categories

Funding

  1. Human Frontiers Science Project [RGP0063/2013]
  2. National Institute of Health (NIH) [GM116423, GM110501, GM55302, P41GM103393]
  3. Department of Energy (DOE), Office of Science, Office of Basic Energy Sciences (OBES) [DE-AC02-05CH11231, DE-AC02-76SF00515]
  4. Federal Ministry of Education and Research (BMBF) [05K12CB4]
  5. European Community [PCIG10-GA-2011-297905]
  6. Helmholtz Virtual Institute Dynamic Pathways in Multidimensional Landscapes
  7. LCLS
  8. Stanford University through the Stanford Institute for Materials Energy Sciences (SIMES)
  9. Lawrence Berkeley National Laboratory (LBNL)
  10. University of Hamburg through the BMBF [FSP 301]
  11. Center for Free Electron Laser Science (CFEL)
  12. U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences [DE-AC02-76SF00515]
  13. DOE Office of Biological and Environmental Research
  14. National Institutes of Health, National Institute of General Medical Sciences [P41GM103393]

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X-ray free electron lasers (XFELs) enable unprecedented new ways to study the electronic structure and dynamics of transition metal systems. L-edge absorption spectroscopy is a powerful technique for such studies and the feasibility of this method at XFELs for solutions and solids has been demonstrated. However, the required x-ray bandwidth is an order of magnitude narrower than that of self-amplified spontaneous emission (SASE), and additional monochromatization is needed. Here we compare L-edge x-ray absorption spectroscopy (XAS) of a prototypical transition metal system based on monochromatizing the SASE radiation of the linac coherent light source (LCLS) with a new technique based on self-seeding of LCLS. We demonstrate how L-edge XAS can be performed using the self-seeding scheme without the need of an additional beam line monochromator. We show how the spectral shape and pulse energy depend on the undulator setup and how this affects the x-ray spectroscopy measurements. (C) 2016 Optical Society of America

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