% IMPORTANT: The following is UTF-8 encoded.  This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.

@ARTICLE{Telesca:864235,
      author       = {Telesca, G. and Ivanova-Stanik, I. and Zagórski, R. and
                      Brezinsek, S. and Carvalho, P. J. and Czarnecka, A. and
                      Giroud, C. and Huber, A. and Lerche, E. and Wiesen, S.},
      title        = {{COREDIV} numerical simulation of high neutron rate
                      {JET}-{ILW} {DD} pulses in view of extension to {JET}-{ILW}
                      {DT} experiments},
      journal      = {Nuclear fusion},
      volume       = {59},
      number       = {5},
      issn         = {1741-4326},
      address      = {Vienna},
      publisher    = {IAEA},
      reportid     = {FZJ-2019-04069},
      pages        = {056026 -},
      year         = {2019},
      abstract     = {Two high performance JET-ILW pulses, pertaining to the 2016
                      experimental campaign, have been numerically simulated with
                      the self-consistent code COREDIV with the aim of predicting
                      the ELM-averaged power load to the target when extrapolated
                      to DT plasmas. The input power of about 33 MW as well as the
                      total radiated power and the average density are similar in
                      the two pulses, but for one of them the density is provided
                      by combined low gas puff and pellet injection, characterized
                      by low SOL density, for the other one by gas fuelling only,
                      at higher SOL density. Considering the magnetic
                      configuration of theses pulses and the presence of a
                      significant amount of Ni (not included in the version of the
                      code used for these simulations), a number of assumptions
                      are made in order to reproduce numerically the main core and
                      SOL experimental data. The extrapolation to DT plasmas at
                      the original input power of 33 MW, and taking into account
                      only the thermal component of the alpha-power, does not show
                      any significant difference regarding the power to the target
                      with respect to the DD case. In contrast, the simulations at
                      auxiliary power 40 MW, both at the original I
                      p  =  3 MA and at I p  =  4 MA, show that
                      the power to the target for both pulses is possibly too high
                      to be sustained for about 5 s by strike-point sweeping
                      alone without any control by Ne seeding. Even though the
                      target power load may decrease to about 13–15 MW with
                      substantial Ne seeding for both pulses, as from numerical
                      predictions, there are indications suggesting that the
                      control of the power load may be more critical for the pulse
                      with pellet injection, due to the reduced SOL radiation.},
      cin          = {IEK-4},
      ddc          = {620},
      cid          = {I:(DE-Juel1)IEK-4-20101013},
      pnm          = {174 - Plasma-Wall-Interaction (POF3-174)},
      pid          = {G:(DE-HGF)POF3-174},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000464453100002},
      doi          = {10.1088/1741-4326/ab0c47},
      url          = {https://juser.fz-juelich.de/record/864235},
}