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@ARTICLE{Klimov:201912,
      author       = {Klimov, N. and Podkovyrov, V. and Zhitlukhin, A. and
                      Kovalenko, D. and Linke, J. and Pintsuk, G. and Landman, I.
                      and Pestchanyi, S. and Bazylev, B. and Janeschitz, G. and
                      Loarte, A. and Merola, M. and Hirai, T. and Federici, G. and
                      Riccardi, B. and Mazul, I. and Giniyatulin, R. and
                      Khimchenko, L. and Koidan, V.},
      title        = {{E}xperimental study of {PFC}s erosion and eroded material
                      deposition under {ITER}-like transient loads at the plasma
                      gun facility {QSPA}-{T}},
      journal      = {Journal of nuclear materials},
      volume       = {415},
      number       = {1},
      issn         = {0022-3115},
      address      = {Amsterdam [u.a.]},
      publisher    = {Elsevier Science},
      reportid     = {FZJ-2015-04202},
      pages        = {S59 - S64},
      year         = {2011},
      abstract     = {The paper concerns experimental investigations of plasma
                      facing components erosion under the plasma heat loads
                      expected in ITER divertor during transient events such as
                      the Type I Edge-Localized Modes and the disruptions. The
                      experiments were carried out at the TRINITI plasma gun
                      QSPA-T. The carbon fiber composite and tungsten macrobrush
                      targets designed for ITER were exposed to multiple plasma
                      pulses of duration 0.5 ms and deposited energy in the range
                      of 0.2–2.5 MJ/m2. Between some of the pulses the eroded
                      surface was analyzed with profilometric measurements and
                      electron microscopy. The CFC erosion is determined mainly by
                      damages to the PAN-fibers. While the energy increases from
                      0.2 to 2.4 MJ/m2 the removed layer of PAN-fibers area
                      increases from 0.01 to 10 μm per pulse. The erosion of
                      tungsten (pure and lanthanum oxide-doped tungsten) is shown
                      to be determined mainly by crack formation, melt layer
                      movement and droplets ejection.},
      cin          = {IEK-2 / N-M},
      ddc          = {530},
      cid          = {I:(DE-Juel1)IEK-2-20101013 / I:(DE-Juel1)N-M-20100415},
      pnm          = {135 - Plasma-wall interactions (POF2-135)},
      pid          = {G:(DE-HGF)POF2-135},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000298128100011},
      doi          = {10.1016/j.jnucmat.2011.01.013},
      url          = {https://juser.fz-juelich.de/record/201912},
}