4.2 Article

Time zero determination for FEL pump-probe studies based on ultrafast melting of bismuth

Journal

STRUCTURAL DYNAMICS-US
Volume 4, Issue 5, Pages -

Publisher

AMER INST PHYSICS
DOI: 10.1063/1.4999701

Keywords

-

Funding

  1. Max Planck Society
  2. Natural Sciences and Engineering Research Council of Canada (NSERC)
  3. Canadian Institute for Advanced Research
  4. X-ray Free Electron Laser Utilization Research Project
  5. Ministry of Education, Culture, Sports, Science, and Technology of Japan (MEXT)
  6. excellence cluster The Hamburg Centre for Ultrafast Imaging - Structure, Dynamics and Control of Matter at the Atomic Scale of the Deutsche Forschungsgemeinschaft
  7. People Programme (Marie Curie Actions) of the European Union's Seventh Framework Programme under REA [623994]
  8. Grants-in-Aid for Scientific Research [17H06141] Funding Source: KAKEN

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A common challenge for pump-probe studies of structural dynamics at X-ray free-electron lasers (XFELs) is the determination of time zero (T-0)-the time an optical pulse (e.g., an optical laser) arrives coincidently with the probe pulse (e.g., a XFEL pulse) at the sample position. In some cases, T-0 might be extracted from the structural dynamics of the sample's observed response itself, but generally, an independent robust method is required or would be superior to the inferred determination of T-0. In this paper, we present how the structural dynamics in ultrafast melting of bismuth can be exploited for a quickly performed, reliable and accurate determination of T-0 with a precision below 20 fs and an overall experimental accuracy of 50 fs to 150 fs (estimated). Our approach is potentially useful and applicable for fixed-target XFEL experiments, such as serial femtosecond crystallography, utilizing an optical pump pulse in the ultraviolet to near infrared spectral range and a pixelated 2D photon detector for recording crystallographic diffraction patterns in transmission geometry. In comparison to many other suitable approaches, our method is fairly independent of the pumping wavelength (UV-IR) as well as of the X-ray energy and offers a favorable signal contrast. The technique is exploitable not only for the determination of temporal characteristics of the experiment at the interaction point but also for investigating important conditions affecting experimental control such as spatial overlap and beam spot sizes. (C) 2017 Author(s).

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