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Publication
Featured researches published by J.M. Kwon.
Nuclear Fusion | 2013
Y.J. Shi; W.H. Ko; J.M. Kwon; P. H. Diamond; S.G. Lee; S.H. Ko; Lu Wang; S. Yi; K. Ida; L. Terzolo; S.W. Yoon; K.D. Lee; J.H. Lee; U.N. Nam; Y.S. Bae; Y.K. Oh; J.G. Kwak; M. Bitter; K. W. Hill; Ö. D. Gürcan; T.S. Hahm
Toroidal rotation profiles have been investigated in KSTAR H-mode plasma using combined auxiliary heating by co-neutral beam injection (NBI) and electron cyclotron resonance heating (ECH). The ion temperature and toroidal rotation are measured with x-ray imaging crystal spectroscopy and charge exchange recombination spectroscopy. H-mode plasma is achieved using co-current 1.3 MW NBI, and a 0.35 MW ECH pulse is added to the flat-top of H-mode. The core rotation profiles, which are centrally peaked in the pure NBI heating phase, flatten when ECH is injected, while the edge pedestal is unchanged. Dramatic decreases in the core toroidal rotation values (ΔVtor/Vtor ~ −30%) are observed when on-axis ECH is added to H-mode. The experimental data show that the decrease of core rotation velocity and its gradient are correlated with the increase of core electron temperature and its gradient, and also with the likely steepening of the density gradient. We thus explore the viability of a hypothesized ITG (ITG ion temperature gradient instability) → TEM (trapped electron mode instability) transition as the explanation of the observed counter-current flow induced by ECH. However, the results of linear microstability analyses using inferred profiles suggest that the TEM is excited only in the deep core, so the viability of the hypothesized explanation is not yet clear.
Physics of Plasmas | 2014
Janghoon Seo; C.S. Chang; S. Ku; J.M. Kwon; Wonho Choe; Stefan H. Müller
Fluid Reynolds stress from turbulence has usually been considered to be responsible for the anomalous toroidal momentum transport in tokamak plasma. Experiment by Muller et al. [Phys. Rev. Lett. 106, 115001 (2011)], however, reported that neither the observed edge rotation profile nor the inward momentum transport phenomenon at the edge region of an H-mode plasma could be explained by the fluid Reynolds stress measured with reciprocating Langmuir-probe. The full-function gyrokinetic code XGC1 is used to explain, for the first time, Muller et al.s experimental observations. It is discovered that, unlike in the plasma core, the fluid Reynolds stress from turbulence is not sufficient for momentum transport physics in plasma edge. The “turbulent neoclassical” physics arising from the interaction between kinetic neoclassical orbit dynamics and plasma turbulence is key in the tokamak edge region across the plasma pedestal into core.
Nuclear Fusion | 2015
Won-Ha Ko; S.H. Ko; J.M. Kwon; P. H. Diamond; K. Ida; Y.M. Jeon; J.H. Lee; S.W. Yoon; J.G. Kwak
The structure and evolution of the ion temperature () and toroidal rotation () profile have been investigated in neutral beam injection (NBI)-heated KSTAR H-mode plasmas, both without and with resonant magnetic pertubations (RMPs). A clear disparity between the width of the -pedestal and that of the -pedestal was observed. Also, it was found that there exists a close correlation and weak relative hysteresis between the pedestal and during both L → H and H → L transitions. During the L → H transition, the -pedestal is observed to form ahead of the -pedestal, and build inward from the separatrix. Linear gyrokinetic stability analysis of these KSTAR profiles was performed. The results indicate that parallel velocity shear is a relevant drive for pedestal turbulence and transport. This was largely ignored in previous studies of the pedestal micro-stability. Pedestal ion temperature and rotation profiles were also measured during edge localized mode (ELM) suppression experiments on KSTAR using an n = 1 RMPs. It was found that the top values of the ion temperature and toroidal rotation pedestal drop with RMPs when ELMs are suppressed.
Nuclear Fusion | 2017
M.J. Choi; Jayhyun Kim; J.M. Kwon; Hyeon K. Park; Y. In; Woochang Lee; Kyeong-Woo Lee; Gunsu S. Yun; Jaehyun Lee; Minwoo Kim; W.H. Ko; Jongha Lee; Y.S. Park; Yong-Su Na; N.C. Luhmann; Byung-Hyuk Park
Multiscale interaction between the magnetic island and turbulence has been demonstrated through simultaneous two-dimensional measurements of turbulence and temperature and flow profiles. The magnetic island and turbulence mutually interact via the coupling between the electron temperature (
Physics of Plasmas | 2014
S. Yi; J.M. Kwon; P. H. Diamond; T. S. Hahm
T_e
Nuclear Fusion | 2016
Y.J. Shi; S.H. Ko; J.M. Kwon; W.H. Ko; P. H. Diamond; S. Yi; K. Ida; K.D. Lee; J.H. Jeong; S.H. Seo; S.H. Hahn; S.W. Yoon; Y.S. Bae; L. Terzolo; G.S. Yun; M. Bitter; K. W. Hill
) gradient, the
Nuclear Fusion | 2015
S. Yi; J.M. Kwon; P. H. Diamond; T.S. Hahm
T_e
Physics of Plasmas | 2018
Wai Ming Lee; J.M. Kwon; S. H. Ko; J. Leem; G.S. Yun; Hyeon K. Park; Y.S. Park; K. W. Kim; N. C. LuhmannJr.; Kstar Team
turbulence, and the poloidal flow. The
Physics of Plasmas | 2017
Kyuho Kim; J.M. Kwon; Choong-Seock Chang; Janghoon Seo; S. Ku; Wonho Choe
T_e
Physics of Plasmas | 2016
S. H. Ko; J.M. Kwon; W.H. Ko; S. S. Kim; H. Jhang; L. Terzolo
gradient altered by the magnetic island is peaked outside and flattened inside the island. The