Intrinsic rotation reversal, non-local transport, and turbulence transition in KSTAR L-mode plasmas

Experiments of electron cyclotron resonance heating (ECH) power scan in KSTAR tokamak clearly demonstrate that both the cutoff density for non-local heat transport (NLT) and the threshold density for intrinsic rotation reversal can be determined by the collisionality. We demonstrate that NLT can be affected by ECH, and the intrinsic rotation direction follows the changes of NLT. The cutoff density of NLT and threshold density for rotation reversal can be significantly increased by ECH. The poloidal flow of turbulence in core plasma is in the electron and the ion diamagnetic direction in ECH plasmas and high density OH plasma, respectively. The auto-power spectra of density fluctuation are almost the same in the outer region for both ECH and OH plasmas. On the other hand, the divergence in density fluctuation spectra at high frequency range between OH and ECH plasma is clearly observed in core region. The features of linear confinement and saturated confinement also appeared in ECH plasma, which is similar to the linear ohmic confinement (LOC) mode and saturate ohmic confinement (SOC) mode. All these observations in macroscopic parameters and micro fluctuations suggest a possible link between the macro phenomena and the structural changes in turbulence mode.

[1]  S. G. Lee,et al.  The first experimental results from x-ray imaging crystal spectrometer for KSTAR. , 2010, The Review of scientific instruments.

[2]  P. Diamond,et al.  Intrinsic torque reversals induced by magnetic shear effects on the turbulence spectrum in tokamak plasmasa) , 2015 .

[3]  E. D. Fredrickson,et al.  CORRIGENDUM: Non-local component of electron heat transport in TFTR , 1996 .

[4]  C. Gil,et al.  Edge cooling experiments and non-local transport phenomena in Tore Supra , 2000 .

[5]  Z. Cui,et al.  Plasma behaviour with molecular beam injection in the HL-1M tokamak , 1998 .

[6]  J. Rice,et al.  Intrinsic rotation in DIII-D , 2006 .

[7]  F. Casson,et al.  Intrinsic toroidal rotation, density peaking, and turbulence regimes in the core of tokamak plasmas. , 2011, Physical review letters.

[8]  C. Domier,et al.  Development of KSTAR ECE imaging system for measurement of temperature fluctuations and edge density fluctuations. , 2010, The Review of scientific instruments.

[9]  S. G. Lee,et al.  Physics and Experimental Results of KSTAR ECH , 2014 .

[10]  D. Seo,et al.  Charge exchange spectroscopy system calibration for ion temperature measurement in KSTAR. , 2010, The Review of scientific instruments.

[11]  P. Diamond,et al.  Neoclassical poloidal and toroidal rotation in tokamaks , 1991 .

[12]  J. Stober,et al.  Propagation of Cold Pulses and Heat Pulses in ASDEX Upgrade , 2000 .

[13]  G. Hogeweij,et al.  Nonlocal Transient Transport and Thermal Barriers in Rijnhuizen Tokamak Project Plasmas , 1999 .

[14]  F. Jenko,et al.  Understanding of the density profile shape, electron heat transport and internal transport barriers observed in ASDEX Upgrade , 2005 .

[15]  C. Gil,et al.  Co- and counter-current rotation in Tore Supra lower hybrid current drive plasmas , 2014 .

[16]  S. Murakami,et al.  Study of toroidal flow generation by ion cyclotron range of frequency minority heating in the Alcator C-Mod plasma , 2016 .

[17]  Yong Chu,et al.  Control and operation of the gas injection systems for KSTAR tokamak , 2013 .

[18]  S. G. Lee,et al.  Effects of electron-cyclotron-resonance-heating-induced internal kink mode on the toroidal rotation in the KSTAR Tokamak. , 2012, Physical review letters.

[19]  B. Duval,et al.  Rotation reversal bifurcation and energy confinement saturation in tokamak Ohmic L-mode plasmas. , 2011, Physical review letters.

[20]  B. Duval,et al.  Observation of spontaneous toroidal rotation inversion in Ohmically heated Tokamak plasmas. , 2006, Physical review letters.

[21]  Volker Naulin,et al.  Transport of parallel momentum by collisionless drift wave turbulence , 2008 .

[22]  K. Kawahata,et al.  Observation of core electron temperature rise in response to an edge cooling in toroidal helical plasmas , 2005 .

[23]  J. Rasmussen,et al.  Cold pulse and rotation reversals with turbulence spreading and residual stress , 2016 .

[24]  S. G. Lee,et al.  Effects of neoclassical toroidal viscosity induced by the intrinsic error fields and toroidal field ripple on the toroidal rotation in tokamaks , 2016 .

[25]  J. H. Schultz,et al.  The KSTAR project: An advanced steady state superconducting tokamak experiment , 2000 .

[26]  K. Shaing Magnetohydrodynamic-activity-induced toroidal momentum dissipation in collisionless regimes in tokamaks , 2003 .

[27]  Fukun Liu,et al.  Observation of cocurrent toroidal rotation in the EAST tokamak with lower-hybrid current drive. , 2011, Physical review letters.

[28]  R. Budny,et al.  Perturbative transport experiments in JET low or reverse magnetic shear plasmas* Perturbative transp , 2002 .

[29]  A. Wootton,et al.  Effects of limited spatial resolution on fluctuation measurements (invited) , 1995 .

[30]  J. Lee,et al.  Development of KSTAR Thomson scattering system. , 2010, The Review of scientific instruments.

[31]  S. Okamura,et al.  Observation of toroidal flow antiparallel to the drift direction in the hot electron mode plasmas in the compact helical system. , 2001, Physical review letters.

[32]  K. D. Lee,et al.  E × B flow velocity deduced from the poloidal motion of fluctuation patterns in neutral beam injected L-mode plasmas on KSTAR , 2016 .

[33]  Rowan,et al.  Strong nonlocal effects in a tokamak perturbative transport experiment. , 1995, Physical review letters.

[34]  R. Waltz,et al.  Anomalous transport scaling in the DIII-D tokamak matched by supercomputer simulation. , 2003, Physical review letters.

[35]  K. D. Lee,et al.  Electron cyclotron emission diagnostics on KSTAR tokamak. , 2010, The Review of scientific instruments.