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@ARTICLE{Borodin:891433,
      author       = {Borodin, D. and Romazanov, J. and Pitts, R. A. and Lisgo,
                      S. W. and Brezinsek, S. and Borodkina, I. and Eksaeva, Alina
                      and Safi, E. and Nordlund, K. and Kirschner, A. and
                      Linsmeier, Ch.},
      title        = {{I}mproved {ERO} modelling of beryllium erosion at {ITER}
                      upper first wall panel using {JET}-{ILW} and {PISCES}-{B}
                      experience},
      journal      = {Nuclear materials and energy},
      volume       = {19},
      issn         = {2352-1791},
      address      = {Amsterdam [u.a.]},
      publisher    = {Elsevier},
      reportid     = {FZJ-2021-01518},
      pages        = {510 - 515},
      year         = {2019},
      abstract     = {ERO is a 3D Monte-Carlo impurity transport and
                      plasma-surface interaction code. In 2011 it was applied for
                      the ITER first wall (FW) life time predictions [1] (critical
                      blanket module BM11). After that the same code was
                      significantly improved during its application to existing
                      fusion-relevant plasma devices: the tokamak JET equipped
                      with an ITER-like wall and linear plasma device PISCES-B.
                      This has allowed testing the sputtering data for beryllium
                      (Be) and showing that the “ERO-min” fit based on the
                      large $(50\%)$ deuterium (D) surface content is well
                      suitable for plasma-wetted areas (D plasma). The improved
                      procedure for calculating of the effective sputtering yields
                      for each location along the plasma-facing surface using the
                      recently developed semi-analytical sheath approach was
                      validated. The re-evaluation of the effective yields for
                      BM11 following the similar revisit of the JET data has
                      indicated significant increase of erosion and motivated the
                      current re-visit of ERO simulations.},
      cin          = {IEK-4},
      ddc          = {624},
      cid          = {I:(DE-Juel1)IEK-4-20101013},
      pnm          = {134 - Plasma-Wand-Wechselwirkung (POF4-134)},
      pid          = {G:(DE-HGF)POF4-134},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000470746100080},
      doi          = {10.1016/j.nme.2019.03.016},
      url          = {https://juser.fz-juelich.de/record/891433},
}