% 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{Klimov:837695,
      author       = {Klimov, N. S. and Putrik, A. B. and Linke, J. and Pitts, R.
                      A. and Zhitlukhin, A. M. and Kuprianov, I. B. and Spitsyn,
                      A. V. and Ogorodnikova, O. V. and Podkovyrov, V. L. and
                      Muzichenko, A. D. and Ivanov, B. V. and Sergeecheva, Ya. V.
                      and Lesina, I. G. and Kovalenko, D. V. and Barsuk, V. A. and
                      Danilina, N. A. and Bazylev, B. N. and Giniyatulin, R. N.},
      title        = {{P}lasma {F}acing {M}aterials {P}erformance under
                      {ITER}-{R}elevant {M}itigated {D}isruption {P}hotonic {H}eat
                      {L}oads},
      journal      = {Journal of nuclear materials},
      volume       = {463},
      issn         = {0022-3115},
      address      = {Amsterdam [u.a.]},
      publisher    = {Elsevier Science},
      reportid     = {FZJ-2017-06555},
      pages        = {61 - 65},
      year         = {2015},
      abstract     = {PFMs (Plasma-facing materials: ITER grade stainless steel,
                      beryllium, and ferritic–martensitic steels) as well as
                      deposited erosion products of PFCs (Be-like, tungsten, and
                      carbon based) were tested in QSPA under photonic heat loads
                      relevant to those expected from photon radiation during
                      disruptions mitigated by massive gas injection in ITER.
                      Repeated pulses slightly above the melting threshold on the
                      bulk materials eventually lead to a regular,
                      “corrugated” surface, with hills and valleys spaced by
                      0.2–2 mm. The results indicate that hill growth (growth
                      rate of ∼1 μm per pulse) and sample thinning in the
                      valleys is a result of melt-layer redistribution. The
                      measurements on the 316L(N)-IG indicate that the amount of
                      tritium absorbed by the sample from the gas phase
                      significantly increases with pulse number as well as the
                      modified layer thickness. Repeated pulses significantly
                      below the melting threshold on the deposited erosion
                      products lead to a decrease of hydrogen isotopes trapped
                      during the deposition of the eroded material.},
      cin          = {IEK-2},
      ddc          = {530},
      cid          = {I:(DE-Juel1)IEK-2-20101013},
      pnm          = {174 - Plasma-Wall-Interaction (POF3-174)},
      pid          = {G:(DE-HGF)POF3-174},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000358467200009},
      doi          = {10.1016/j.jnucmat.2014.11.098},
      url          = {https://juser.fz-juelich.de/record/837695},
}