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@ARTICLE{Wunderer:207193,
      author       = {Wunderer, C. B. and Marras, A. and Bayer, M. and Glaser, L.
                      and Göttlicher, P. and Lange, S. and Pithan, F. and Scholz,
                      F. and Seltmann, J. and Shevyakov, I. and Smoljanin, S. and
                      Viefhaus, J. and Viti, M. and Xia, Q. and Zimmer, M. and
                      Klumpp, S. and Gasiorek, P. and Guerrini, N. and Marsh, B.
                      and Sedgwick, I. and Turchetta, R. and Cautero, G. and
                      Farina, S. and Giuressi, D. and Menk, R. and Stebel, L. and
                      Yousef, H. and Marchal, J. and Nicholls, T. and Tartoni, N.
                      and Graafsma, H.},
      title        = {{T}he {PERCIVAL} {S}oft {X}-{R}ay {I}mager},
      journal      = {Journal of Instrumentation},
      volume       = {9},
      issn         = {1748-0221},
      address      = {London},
      publisher    = {Inst. of Physics},
      reportid     = {PUBDB-2015-01177},
      pages        = {C03056},
      year         = {2014},
      note         = {OA},
      abstract     = {With the increased brilliance of state-of-the-art
                      Synchrotron radiation sources and the advent of Free
                      Electron Lasers enabling revolutionary science with EUV to
                      X-ray photons comes an urgent need for suitable photon
                      imaging detectors. Requirements include high frame rates,
                      very large dynamic range, single-photon counting capability
                      with low probability of false positives, and
                      (multi)-megapixels.PERCIVAL (``Pixelated Energy Resolving
                      CMOS Imager, Versatile and Large'') is currently being
                      developed by a collaboration of DESY, RAL, Elettra and DLS
                      to address this need for the soft X-ray regime. PERCIVAL is
                      a monolithic active pixel sensor (MAPS), i.e. based on CMOS
                      technology. It will be back-thinned to access its primary
                      energy range of 250 eV to 1 keV with target efficiencies
                      above $90\%.$ According to its preliminary specifications,
                      the roughly 10 × 10 cm2, 3520 × 3710 pixel monolithic
                      sensor will operate at frame rates up to 120 Hz
                      (commensurate with most FELs) and use multiple gains within
                      its 27 μm pixels to measure (e.g. at 500 eV) 1 to ~ 105
                      simultaneously-arriving photons.Currently, small-scale
                      front-illuminated prototype systems (160 × 210 pixels) are
                      undergoing detailed testing with visible-light as well as
                      X-ray photons.},
      month         = {Jun},
      date          = {2013-06-23},
      organization  = {15th International Workshop on
                       Radiation Imaging Detectors, Paris
                       (France), 23 Jun 2013 - 27 Jun 2013},
      cin          = {FS-PE / FS-DS / DOOR / UNI/EXP / FS-SCS},
      ddc          = {610},
      cid          = {I:(DE-H253)FS-PE-20120731 / I:(DE-H253)FS-DS-20120731 /
                      I:(DE-H253)HAS-User-20120731 / $I:(DE-H253)UNI_EXP-20120731$
                      / I:(DE-H253)FS-SCS-20131031},
      pnm          = {PETRA Beamline P04 (POF2-54G14)},
      pid          = {G:(DE-H253)POF2-P04-20130405},
      experiment   = {EXP:(DE-H253)P-P04-20150101},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000336123200056},
      doi          = {10.1088/1748-0221/9/03/C03056},
      url          = {https://bib-pubdb1.desy.de/record/207193},
}