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@ARTICLE{Rosato:7943,
      author       = {Rosato, J. and Marandet, Y. and Capes, H. and Ferri, S. and
                      Mossé, C. and Godbert-Mouret, L. and Koubiti, M. and Stamm,
                      R.},
      title        = {{S}tark broadening of hydrogen lines in low-density
                      magnetized plasmas},
      journal      = {Physical review / E},
      volume       = {79},
      number       = {4},
      issn         = {1539-3755},
      address      = {College Park, Md.},
      publisher    = {APS},
      reportid     = {PreJuSER-7943},
      pages        = {046408},
      year         = {2009},
      note         = {This work was partially supported by the project "Radiation
                      Absorption Effects" of the French Federation de Recherche
                      sur la Fusion Magnetique, by the project "PHOTONITER" of the
                      French Agence Nationale de la Recherche (Contract No.
                      ANR-07-BLAN-0187-01), and by the collaboration LRC DSM 99-14
                      (PIIM/CEA Cadarache)},
      abstract     = {Stark broadening of hydrogen lines in the presence of a
                      magnetic field is revisited, with emphasis on the role of
                      the ion component under typical conditions of magnetized
                      fusion devices. An impact theory for ions valid at low
                      density (N-e less than or similar to 10(14) cm(-3)) and
                      taking into account the Zeeman degeneracy removal of the
                      atomic states is developed. It is shown that the Stark
                      widths of the Lorentz triplet components strongly depend on
                      the magnetic field. The model is validated by a computer
                      simulation method. For the lateral sigma components of Ly
                      alpha, we show that the impact approximation still holds for
                      densities as high as N-e similar to 10(15) cm(-3). In
                      contrast, for the central pi component as well as for the
                      other lines from low principal quantum number, significant
                      discrepancies between the proposed theory and the simulation
                      results appear at high density. Application to D alpha in
                      tokamak divertor plasma conditions shows that, in this case,
                      the quasistatic approximation becomes more relevant.},
      keywords     = {J (WoSType)},
      cin          = {IEF-4},
      ddc          = {530},
      cid          = {I:(DE-Juel1)VDB812},
      pnm          = {Fusion},
      pid          = {G:(DE-Juel1)FUEK403},
      shelfmark    = {Physics, Fluids $\&$ Plasmas / Physics, Mathematical},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000265941400076},
      doi          = {10.1103/PhysRevE.79.046408},
      url          = {https://juser.fz-juelich.de/record/7943},
}