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@ARTICLE{Jia:836424,
      author       = {Jia, M. and Zang, Q. and Liu, Y. Q. and Guo, W. and Gu, S.
                      and Lyu, B. and Zhao, H. and Li, G. and Qian, J. and Chu, N.
                      and Wang, H. H. and Shi, T. and He, K. and Shen, B. and
                      Gong, X. and Ji, X. and Qi, M. and Yuan, Q. and Sheng, Z.
                      and Gao, G. and Song, Y. and Fu, P. and Wan, B. and Sun, Y.
                      and Wang, S. and Chen, D. and Xu, L. and Zhang, T. and Liu,
                      Y. and Li, Yun and Yang, X. and Liang, Yunfeng and Wang, L.},
      title        = {{E}dge localized mode control using n   =  1
                      resonant magnetic perturbation in the {EAST} tokamak},
      journal      = {Nuclear fusion},
      volume       = {57},
      number       = {3},
      issn         = {1741-4326},
      address      = {Vienna},
      publisher    = {IAEA},
      reportid     = {FZJ-2017-05545},
      pages        = {036007 -},
      year         = {2017},
      abstract     = {A set of in-vessel resonant magnetic perturbation (RMP)
                      coil has been recently installed in EAST. It can generate a
                      range of spectrum, and there is a relatively large window
                      for edge localized mode (ELM) control according to the
                      vacuum field modeling of the edge magnetic island
                      overlapping area. Observation of mitigation and suppression
                      of ELM in slow rotating plasmas during the application of an
                      n  =  1 RMP is presented in this paper. Strong ELM
                      mitigation effect is observed in neutral beam injection
                      heating plasmas. The ELM frequency increases by a factor of
                      5, and the crash amplitude and the particle flux are
                      effectively reduced by a similar factor. Clear density
                      pump-out and magnetic braking effects are observed during
                      the application of RMP. Footprint splitting is observed
                      during ELM mitigation and agrees well with vacuum field
                      modelling. Strong ELM mitigation happens after a second
                      sudden drop of plasma density, which indicates the possible
                      effect due to field penetration of the resonant harmonics
                      near the pedestal top, where the electron perpendicular
                      rotation becomes flat and close to zero after the
                      application of RMP. ELM suppression is achieved in a
                      resonant window during the scan of the n  =  1 RMP
                      spectrum in radio-frequency (RF) dominant heating plasmas.
                      The best spectrum for ELM suppression is consistent with the
                      resonant peak of RMP by taking into account of linear
                      magnetohydrodynamics plasma response. There is no mode
                      locking during the application of n  =  1 RMP in
                      ELMy H-mode plasmas, although the maximal coil current is
                      applied.},
      cin          = {IEK-4},
      ddc          = {530},
      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:000390769600007},
      doi          = {10.1088/1741-4326/57/3/036007},
      url          = {https://juser.fz-juelich.de/record/836424},
}