Progress of the KSTAR Research Program Exploring the Advanced High Performance and Steady-State Plasma Operations

Korea Superconducting Tokamak Advanced Research (KSTAR) program is strongly focused on solving the scientific and technological issues in steady-state high performance plasma operation in preparation for ITER operation as well as the design basis for DEMO. In this regards, KSTAR has made significant advances in developing long pulse and high performance plasma scenarios utilizing the advantage of the fully superconducting tokamak. Ten-year of KSTAR operation showed the outstanding progress in the plasma control extending the operation window of the plasma discharges achieving the H-mode up to 1 MA in plasma current, up to 72 s in flat top duration, and up to 2.16 in elongation. In addition to the long pulse discharge, high performance discharges with high betas (βN ~ 3) could be achieved in the broad range of edge safety factor (q95) without external error field correction. The unique features of the KSTAR device (magnetic accuracy with extremely low error fields, steady-state capable heating systems, in-vessel control coils, and advanced imaging and profile diagnostics) has been fully exploited to explore the unveiled physics as well as to exploring the systematic solution for suppression of edge localized mode (ELM) crash. Achieved examples are the record long pulse of H-mode operation without an ELM crash (~ 30 s up to date), and progress in the fundamental transport physics through systematic study using these unique capabilities. Based on the previous research results, intensive research will be followed to explore the advanced high beta operation (βN ~ 4) with fully suppressed harmful MHD instabilities aiming the integrated solution for DEMO. In this regards, an additional current drive systems and in-vessel structures will be upgraded.

[1]  K. Tanaka,et al.  Development of multi-channel electron spectrometer. , 2010, The Review of scientific instruments.

[2]  Wonho Choe,et al.  Comparison of divertor heat flux splitting by 3D fields with field line tracing simulation in KSTAR , 2017 .

[3]  H. L. Yang,et al.  Design of neutral beam injection system for KSTAR tokamak , 2011 .

[4]  George H. Neilson,et al.  A preliminary conceptual design study for Korean fusion DEMO reactor , 2013 .

[5]  Jong-Ho Sun,et al.  Initial phase wall conditioning in KSTAR , 2011 .

[6]  Seungtae Oh,et al.  Tomographic reconstruction of two-dimensional radiated power distribution during impurity injection in KSTAR plasmas using an infrared imaging video bolometer , 2018 .

[7]  Seong-Heon Seo The electron density profile measurement with a fast time-resolution in the KSTAR tokamak , 2014 .

[8]  S. Jeong,et al.  Design of a heterodyne electron cyclotron emission system on KSTAR , 2003 .

[9]  Hogun Jhang,et al.  A statistical analysis of avalanching heat transport in stationary enhanced core confinement regimes , 2012 .

[10]  Patrick H. Worley,et al.  A fast low-to-high confinement mode bifurcation dynamics in the boundary-plasma gyrokinetic code XGC1 , 2018 .

[11]  McGuire,et al.  Observation of nonlinear neoclassical pressure-gradient-driven tearing modes in TFTR. , 1995, Physical review letters.

[12]  X. Litaudon,et al.  Recent progress on lower hybrid current drive and implications for ITER , 2013, 1503.05047.

[13]  A. Bondeson,et al.  Linear Stability of Resistive MHD Modes , 1994 .

[14]  S. G. Lee,et al.  Rotational resonance of nonaxisymmetric magnetic braking in the KSTAR tokamak. , 2013, Physical review letters.

[15]  B. P. Duval,et al.  Inter-machine comparison of intrinsic toroidal rotation in tokamaks , 2007 .

[16]  Bong Guen Hong,et al.  Development of a KSTAR ICRF antenna for long pulse operation , 2003 .

[17]  C W Domier,et al.  Appearance and dynamics of helical flux tubes under electron cyclotron resonance heating in the core of KSTAR plasmas. , 2012, Physical review letters.

[18]  O Sauter,et al.  From current-driven to neoclassically driven tearing modes. , 2002, Physical review letters.

[19]  T. Fujita,et al.  Internal transport barrier in tokamak and helical plasmas , 2018 .

[20]  M. Kwon,et al.  Runaway Electron Suppression by ECRH and RMP in KSTAR , 2013 .

[21]  H. Na,et al.  Configuration and installation design of optical diagnostic systems on KSTAR , 2011 .

[22]  Jae-Min Kwon,et al.  Nonlinear Interaction of Edge-Localized Modes and Turbulent Eddies in Toroidal Plasma under n=1 Magnetic Perturbation. , 2016, Physical review letters.

[23]  Kang Wook Kim,et al.  Observation of electron driven quasi-coherent modes and their connection with core intrinsic rotation in KSTAR ECH and ohmic L-mode plasmas , 2018 .

[24]  C. Gormezano,et al.  Review of lower hybrid wave heating and current drive , 1986 .

[25]  Harold P. Furth,et al.  Tearing mode in the cylindrical tokamak , 1973 .

[26]  A. Loarte,et al.  Enhanced understanding of non-axisymmetric intrinsic and controlled field impacts in tokamaks , 2017 .

[27]  A. C. England,et al.  Study on Pre-Ionization Using Second-Harmonic Electron Cyclotron Waves for the KSTAR First Plasma , 2007 .

[28]  Yong-Seok Hwang,et al.  Design and construction of the KSTAR tokamak , 2001 .

[29]  K. D. Lee,et al.  Intrinsic rotation reversal, non-local transport, and turbulence transition in KSTAR L-mode plasmas , 2017 .

[30]  L. L. Lao,et al.  Equilibrium and global MHD stability study of KSTAR high beta plasmas under passive and active mode control , 2010 .

[31]  J. Manickam,et al.  Advances in global MHD mode stabilization research on NSTX , 2010 .

[32]  Min Xu,et al.  Fusion Research and International Collaboration in the Asian Region , 2018 .

[33]  C. Bourdelle,et al.  Quasi-coherent modes and electron-driven turbulence , 2014 .

[34]  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.

[35]  H. S. Kim,et al.  VUV spectroscopy in impurity injection experiments at KSTAR using prototype ITER VUV spectrometer. , 2017, The Review of scientific instruments.

[36]  N. W. Eidietis,et al.  Overview of KSTAR initial operation , 2011 .

[37]  Michio Okabayashi,et al.  Extremely low intrinsic non-axisymmetric field in KSTAR and its implications , 2015 .

[38]  D. Pacella,et al.  Tomographic 2-D X-ray imaging of toroidal fusion plasma using a tangential pinhole camera with gas electron multiplier detector , 2016 .

[39]  Stephen C. Jardin,et al.  A high-order implicit finite element method for integrating the two-fluid magnetohydrodynamic equations in two dimensions , 2007, J. Comput. Phys..

[40]  Gunsu Yun,et al.  Toroidal rotation profile structure in KSTAR L-mode plasmas with mixed heating by NBI and ECH , 2015 .

[41]  Calvin Domier,et al.  Dynamics of multiple flux tubes in sawtoothing KSTAR plasmas heated by electron cyclotron waves: I. Experimental analysis of the tube structure , 2015 .

[42]  H. S. Kim,et al.  Improvements of magnetic measurements for plasma control in KSTAR tokamak , 2017 .

[43]  J Ko,et al.  Diagnostic development for current density profile control at KSTAR , 2016 .

[44]  J. Ko,et al.  Direct measurements of safety factor profiles with motional Stark effect for KSTAR tokamak discharges with internal transport barriers. , 2017, The Review of scientific instruments.

[45]  K. D. Lee,et al.  Formation of the internal transport barrier in KSTAR , 2017 .

[46]  M. Hirsch,et al.  41st EPS Conference on Plasma Physics , 2014 .

[47]  Guillaume Latu,et al.  The $\bf {E × B}$ staircase of magnetised plasmas , 2017 .

[48]  J. G. Bak,et al.  Electric probe diagnostics for measuring SOL parameters, wall and divertor fluxes in KSTAR , 2016 .

[49]  Suk-Kwon Kim,et al.  Resonant loop system for the KSTAR ICRF current drive , 2013 .

[50]  S. C. Jardin,et al.  Investigation of instabilities and rotation alteration in high beta KSTAR plasmas , 2017 .

[51]  Sonjong Wang,et al.  Design and RF test of a prototype traveling wave antenna for helicon current drive in KSTAR , 2018 .

[52]  Yong-Su Na,et al.  Characteristics of the first H-mode discharges in KSTAR , 2011 .

[53]  S. C. Jardin,et al.  Validation of the ‘full reconnection model’ of the sawtooth instability in KSTAR , 2018 .

[54]  Stephen C. Jardin,et al.  Calculations of two-fluid magnetohydrodynamic axisymmetric steady-states , 2009, J. Comput. Phys..

[55]  S. G. Lee,et al.  Observation of the intrinsic rotation in KSTAR Ohmic L-mode plasmas , 2016 .

[56]  Gunter,et al.  Complete suppression of neoclassical tearing modes with current drive at the electron-cyclotron-resonance frequency in ASDEX upgrade tokamak , 2000, Physical review letters.

[57]  Jun Ho Yeom,et al.  Design concept of K-DEMO for near-term implementation , 2015 .

[58]  W. Hooke,et al.  Review of experiments on current drive in Tokamaks by means of RF waves , 1984 .

[59]  K. S. Lee,et al.  Improvement of initial vacuum condition along 2008–2010 KSTAR campaign by vessel baking , 2011 .

[60]  S Zoletnik,et al.  Combined hydrogen and lithium beam emission spectroscopy observation system for Korea Superconducting Tokamak Advanced Research. , 2015, The Review of scientific instruments.

[61]  G S Yun,et al.  Post calibration of the two-dimensional electron cyclotron emission imaging instrument with electron temperature characteristics of the magnetohydrodynamic instabilities. , 2016, The Review of scientific instruments.

[62]  C. D. Beidler,et al.  Current Drive Calculations with an Advanced Adjoint Approach , 2009 .

[63]  Joachim Roth,et al.  Tritium inventory in ITER plasma-facing materials and tritium removal procedures , 2008 .

[64]  S. G. Lee,et al.  Study on the heat flux reconstruction with the infrared thermography for the divertor target plates in the KSTAR tokamak. , 2016, The Review of scientific instruments.

[65]  S. G. Lee,et al.  Validation of Toroidal Rotation and Ion Temperature in KSTAR Plasmas , 2016 .

[66]  Go Matsunaga,et al.  Development of reversed shear plasmas with high bootstrap current fraction towards reactor relevant regime in JT-60U , 2009 .

[67]  T. T. Suzuki,et al.  Stabilization of neoclassical tearing modes by electron cyclotron current drive in JT-60U , 2007 .

[68]  Hyunsun Han,et al.  Suppression of edge localized mode crashes by multi-spectral non-axisymmetric fields in KSTAR , 2017 .

[69]  R Betti,et al.  Resistive wall mode instability at intermediate plasma rotation. , 2010, Physical review letters.

[70]  Myeun Kwon,et al.  Neutron emission from KSTAR Ohmically heated plasmas , 2011 .

[71]  L. L. Lao,et al.  Compatibility of internal transport barrier with steady-state operation in the high bootstrap fraction regime on DIII-D , 2015, Nuclear Fusion.

[72]  John L. Johnson,et al.  Resistive instabilities in general toroidal plasma configurations , 1975 .

[73]  S. G. Lee,et al.  A comprehensive study on rotation reversal in KSTAR: experimental observations and modelling , 2017 .

[74]  T. L. Rhodes,et al.  Suppression of large edge localized modes with edge resonant magnetic fields in high confinement DIII-D plasmas , 2005 .

[75]  Young-chul Ghim,et al.  The design of two color interferometer system for the 3-dimensional analysis of plasma density evolution on KSTAR , 2016 .

[76]  P T Lang,et al.  First observation of edge localized modes mitigation with resonant and nonresonant magnetic perturbations in ASDEX Upgrade. , 2011, Physical review letters.

[77]  R. E. Bell,et al.  Modifications to ideal stability by kinetic effects in NSTX , 2015 .

[78]  G. V. Pereverzev,et al.  TORBEAM, a beam tracing code for electron-cyclotron waves in tokamak plasmas , 2001 .

[79]  S. G. Lee,et al.  Suppression of edge localized modes in high-confinement KSTAR plasmas by nonaxisymmetric magnetic perturbations. , 2012, Physical review letters.

[80]  V. L. Vdovin,et al.  Current generation by helicons and lower hybrid waves in modern tokamaks and reactors ITER and DEMO. Scenarios, modeling and antennae , 2013 .

[81]  Gunsu Yun,et al.  Investigation of MHD instabilities and control in KSTAR preparing for high beta operation , 2013 .

[82]  J. G. Kwak,et al.  Helicon wave coupling in KSTAR plasmas for off-axis current drive in high electron pressure plasmas , 2017 .

[83]  Jin-Seob Kang,et al.  Development of frequency modulation reflectometer for Korea Superconducting Tokamak Advanced Research tokamak. , 2013, The Review of scientific instruments.

[84]  E. J. Strait,et al.  COMPLETE SUPPRESSION OF THE M=2/N-1 NEOCLASSICAL TEARING MODE USING ELECTRON CYCLOTRON CURRENT DRIVE ON DIII-D , 2003 .

[85]  D. A. Humphreys,et al.  Commissioning and initial operation of KSTAR superconducting tokamak , 2009 .

[86]  Robert Hager,et al.  Gyrokinetic simulation study of magnetic island effects on neoclassical physics and micro-instabilities in a realistic KSTAR plasma , 2018 .

[87]  S. G. Lee,et al.  Diagnostics for first plasma and development plan on KSTAR. , 2010, The Review of scientific instruments.

[88]  R. Carrera,et al.  Island bootstrap current modification of the nonlinear dynamics of the tearing mode , 1986 .

[89]  H. L. Yang,et al.  Power supply system for KSTAR neutral beam injector , 2015 .

[90]  Calvin Domier,et al.  Microwave imaging reflectometry for density fluctuation measurement on KSTAR , 2014 .

[91]  Kozo Yamazaki,et al.  Achievement of high fusion triple product, steady-state sustainment and real-time NTM stabilization in high-βp ELMy H-mode discharges in JT-60U , 2003 .

[92]  L. L. Lao,et al.  Development of high poloidal beta, steady-state scenario with ITER-like tungsten divertor on EAST , 2017 .

[93]  S. G. Lee,et al.  Diamagnetic loop measurement in Korea Superconducting Tokamak Advanced Research machine. , 2011, The Review of scientific instruments.

[94]  S. G. Lee,et al.  Investigation of intrinsic toroidal rotation scaling in KSTAR , 2017 .

[95]  N. C. Luhmann,et al.  Multiscale interaction between a large scale magnetic island and small scale turbulence , 2017, 1705.09487.

[96]  C. H. Skinner,et al.  Plasma{material interactions in current tokamaks and their implications for next step fusion reactors , 2001 .