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@ARTICLE{Schwinkendorf:428414,
      author       = {Schwinkendorf, Jan-Patrick and Bohlen, S. and Couperus
                      Cabadağ, J. P. and Ding, H. and Irman, A. and Karsch, S.
                      and Köhler, A. and Krämer, J. M. and Kurz, T. and Kuschel,
                      S. and Osterhoff, J. and Schaper, Lucas and Schinkel, D. and
                      Schramm, U. and Zarini, O. and D'Arcy, R.},
      title        = {{C}harge calibration of {DRZ} scintillation phosphor
                      screens},
      journal      = {Journal of Instrumentation},
      volume       = {14},
      number       = {09},
      issn         = {1748-0221},
      address      = {London},
      publisher    = {Inst. of Physics},
      reportid     = {PUBDB-2019-04565},
      pages        = {P09025 - P09025},
      year         = {2019},
      note         = {(c) IOP Publishing Ltd and Sissa Medialab},
      abstract     = {As a basic diagnostic tool, scintillation screens are
                      employed in particle acceleratorsto detect charged
                      particles. In extension to the recent revision on the
                      calibration of scintillationscreens commonly applied in the
                      context of plasma acceleration [T. Kurz et al.,Rev. Sci.
                      Instrum.89(2018) 093303], here we present the charge
                      calibration of three DRZ screens (Std, Plus, High),
                      whichpromise to offer similar spatial resolution to other
                      screen types whilst reaching higher conversionefficiencies.
                      The calibration was performed at the Electron Linac for
                      beams with high Brilliance andlow Emittance (ELBE) at the
                      Helmholtz-Zentrum Dresden-Rossendorf, which delivers
                      picosecond-long beams of up to 40 MeV energy. Compared to
                      the most sensitive screen, Kodak BioMAX MS,of the
                      aforementioned recent investigation by Kurz et al., the
                      sample with highest yield in thiscampaign, DRZ High,
                      revealed a $30\%$ increase in light yield. The detection
                      threshold with thesescreens was found to be below 10 pC/mm2.
                      For higher charge-densities (several nC/mm2)
                      saturationeffects were observed. In contrast to the recent
                      reported work, the DRZ screens were more
                      robust,demonstrating higher durability under the same high
                      level of charge deposition.},
      cin          = {FLA},
      ddc          = {610},
      cid          = {I:(DE-H253)FLA-20120731},
      pnm          = {631 - Accelerator R $\&$ D (POF3-631) / PWA - Research
                      group for plasma-based accelerators (PWA-20150304) /
                      VH-VI-503 - Plasma wakefield acceleration of highly
                      relativistic electrons with FLASH $(2015_IFV-VH-VI-503)$},
      pid          = {G:(DE-HGF)POF3-631 / G:(DE-H253)PWA-20150304 /
                      $G:(DE-HGF)2015_IFV-VH-VI-503$},
      experiment   = {EXP:(DE-H253)FLASHForward-20150101},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000498531700008},
      doi          = {10.1088/1748-0221/14/09/P09025},
      url          = {https://bib-pubdb1.desy.de/record/428414},
}