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@ARTICLE{MonierGarbet:48298,
      author       = {Monier-Garbet, P. and Andrew, Ph. and Rapp, J. and Belo, P.
                      and Bonheure, G. and Corre, Y. and Crombe, K. and Dumortier,
                      P. and Eich, T. and Felton, R. and Harling, J. and Hogan, J.
                      and Huber, A. and Jachmich, S. and Joffrin, E. and
                      Koslowski, H. R. and Kreter, A. and Maddison, G. and
                      Matthews, G. F. and Messiaen, A. and Nave, M. F. and Ongena,
                      J. and Parail, V. and Puiatti, M. E. and Rapp, J. and
                      Sartori, R. and Stober, J. and Tokar, M. Z. and Unterberg,
                      B. and Valisa, M. and Voitsekhovitch, I. and von Hellermann,
                      M.},
      title        = {{I}mpurity seeded {ELM}y {H}-modes in {JET} with high
                      density and reduced heat load},
      journal      = {Nuclear fusion},
      volume       = {45},
      issn         = {0029-5515},
      address      = {Vienna},
      publisher    = {IAEA},
      reportid     = {PreJuSER-48298},
      pages        = {1404 - 1410},
      year         = {2005},
      note         = {Record converted from VDB: 12.11.2012},
      abstract     = {Experiments performed at JET during the past two years show
                      that, in high triangularity H-mode plasmas with I-p = 2.5
                      MA, n(e)/n(Gr) approximate to 1.0, it is possible to radiate
                      separately up to approximate to $40\%$ of the total injected
                      power on closed flux surfaces in the pedestal region (argon
                      seeding) and up to approximate to $50\%$ of the injected
                      power in the divertor region (nitrogen seeding), while
                      maintaining the confinement improvement factor at the value
                      required for ITER, H98(y, 2) 1.0. The total radiated power
                      fraction achieved in both cases $(65-70\%)$ is close to that
                      required for ITER. However, Type I ELMS observed with
                      impurity seeding have the same characteristics as that
                      observed in reference pulses without seeding: decreasing
                      plasma energy loss per ELM with increasing pedestal
                      collisionality. One has to reach the Type III ELM regime to
                      decrease the transient heat load to the divertor to
                      acceptable values for ITER, although at the expense of
                      confinement. The feasibility of an integrated scenario with
                      Type-III ELMS, and q(95) = 2.6 to compensate for the low H
                      factor, has been demonstrated on JET. This scenario would
                      meet ITER requirements at 17 MA provided that the IPB98
                      scaling for energy content is accurate enough, and provided
                      that a lower dilution is obtained when operating at higher
                      absolute electron density.},
      keywords     = {J (WoSType)},
      cin          = {IPP},
      ddc          = {530},
      cid          = {I:(DE-Juel1)VDB181},
      pnm          = {Kernfusion und Plasmaforschung},
      pid          = {G:(DE-Juel1)FUEK250},
      shelfmark    = {Physics, Fluids $\&$ Plasmas / Physics, Nuclear},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000233679100024},
      doi          = {10.1088/0029-5515/45/11/022},
      url          = {https://juser.fz-juelich.de/record/48298},
}