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

Journal Article · · Optics Express
DOI:https://doi.org/10.1364/OE.24.022469· OSTI ID:1348872
 [1];  [2];  [3];  [4];  [5];  [5];  [6];  [4];  [4];  [4];  [4];  [4];  [4];  [4];  [7];  [8];  [3];  [6];  [6];  [5] more »;  [9];  [10];  [11];  [12];  [12];  [6];  [13];  [3];  [5];  [5];  [3];  [10] « less
  1. SLAC National Accelerator Lab., Menlo Park, CA (United States). Linac Coherent Light Source and Stanford Synchrotron Radiation Lightsource
  2. SLAC National Accelerator Lab., Menlo Park, CA (United States). Linac Coherent Light Source; Lawrence Berkeley National Lab. (LBNL), Berkeley, CA (United States). Molecular Biophysics and Integrated Bioimaging Division
  3. Helmholtz-Zentrum Berlin (HZB), (Germany). German Research Centre for Materials and Energy. Inst. for Methods and Instrumentation for Synchrotron Radiation Research
  4. SLAC National Accelerator Lab., Menlo Park, CA (United States). Linac Coherent Light Source
  5. Lawrence Berkeley National Lab. (LBNL), Berkeley, CA (United States). Molecular Biophysics and Integrated Bioimaging Division
  6. Helmholtz-Zentrum Berlin (HZB), (Germany). German Research Centre for Materials and Energy. Inst. for Nanometer Optics and Technology
  7. SLAC National Accelerator Lab., Menlo Park, CA (United States). Stanford Synchrotron Radiation Lightsource
  8. Helmholtz-Zentrum Berlin (HZB), (Germany). German Research Centre for Materials and Energy. Inst. for Nanometer Optics and Technology; Paul Scherrer Inst. (PSI), Villigen (Switzerland)
  9. Synchrotron SOLEIL, Saint-Aubin (France)
  10. SLAC National Accelerator Lab., Menlo Park, CA (United States). Linac Coherent Light Source and Stanford Pulse Inst.
  11. SLAC National Accelerator Lab., Menlo Park, CA (United States). Stanford Pulse Inst.
  12. Univ. of California, Irvine, CA (United States). Dept. of Chemistry
  13. Helmholtz-Zentrum Berlin (HZB), (Germany). German Research Centre for Materials and Energy. Inst. for Methods and Instrumentation for Synchrotron Radiation Research; Univ. of Potsdam (Germany). Inst. for Physics and Astronomy

© 2016 Optical Society of America. 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.

Research Organization:
SLAC National Accelerator Lab., Menlo Park, CA (United States); Lawrence Berkeley National Lab. (LBNL), Berkeley, CA (United States)
Sponsoring Organization:
USDOE Office of Science (SC), Basic Energy Sciences (BES)
Grant/Contract Number:
05K12CB4; RGP0063/2013; PCIG10-GA-2011-297905; GM110501; GM116423; GM55302; P41GM103393; AC02-05CH11231; AC02-76SF00515
OSTI ID:
1348872
Alternate ID(s):
OSTI ID: 1393084
Journal Information:
Optics Express, Vol. 24, Issue 20; ISSN 1094-4087
Publisher:
Optical Society of America (OSA)Copyright Statement
Country of Publication:
United States
Language:
English
Citation Metrics:
Cited by: 15 works
Citation information provided by
Web of Science

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Cited By (2)

Core-level nonlinear spectroscopy triggered by stochastic X-ray pulses journal October 2019
Probing the oxidation state of transition metal complexes text January 2019

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