Study of correlations between LOC/SOC transition, intrinsic toroidal rotation reversal and TEM/ITG bifurcation with different working gases in TCV

The effects of different working gases on the transition from linear ohmic confinement (LOC) regime to saturated ohmic confinement (SOC) regime and its relation to the intrinsic toroidal rotation reversal phenomenon were explored in the TCV tokamak. The energy confinement saturation was studied across D, H and He density ramps, and a range of ECRH injection power and through variations of ohmic plasma current. The occurrence of rotation reversal, concomitantly with the LOC–SOC transition, was observed only for certain cases, making us formally exclude a causal relation between the two phenomena. A strong correlation between the evolution of toroidal rotation profiles and electron density gradients was, however, observed, in agreement with previous works (Lebschy et al 2017 Nucl. Fusion 58 026013; Hornsby et al 2018 Nucl. Fusion 58 056008). Linear gyrokinetic simulations were performed to probe the turbulent regime of these discharges, showing a dominance of trapped electron mode (TEM) during the LOC phase and a mixture of TEM and ion temperature gradient (ITG) following the transition to SOC regime in D. Such a TEM/ITG bifurcation was less pronounced in H and He. MHD activity was monitored throughout the discharges and possible correlations between sawteeth instability activity, energy confinement time saturation and rotation reversal are highlighted.

[1]  B. Duval,et al.  Upgrade of the neutral beam heating system on the TCV tokamak – second high energy neutral beam , 2023, Fusion engineering and design.

[2]  B. Duval,et al.  Overview of the TCV tokamak experimental programme , 2022, Nuclear Fusion.

[3]  J. Citrin,et al.  Understanding LOC/SOC phenomenology in tokamaks , 2020, Nuclear Fusion.

[4]  Y. Camenen,et al.  Isotope dependence of energy, momentum and particle confinement in tokamaks , 2020, Journal of Plasma Physics.

[5]  P. Diamond,et al.  Evidence and modeling of turbulence bifurcation in L-mode confinement transitions on Alcator C-Mod , 2020, Physics of Plasmas.

[6]  M. Shoji,et al.  Isotope effects on energy, particle transport and turbulence in electron cyclotron resonant heating plasma of the Large Helical Device , 2019, Nuclear Fusion.

[7]  J. Rice,et al.  Hysteresis as a probe of turbulent bifurcation in intrinsic rotation reversals on Alcator C-Mod , 2019, Nuclear Fusion.

[8]  F. Ryter,et al.  Heat transport driven by the ion temperature gradient and electron temperature gradient instabilities in ASDEX Upgrade H-modes , 2019, Nuclear Fusion.

[9]  T. Rhodes,et al.  Main-ion intrinsic toroidal rotation across the ITG/TEM boundary in DIII-D discharges during ohmic and electron cyclotron heating , 2019, Physics of Plasmas.

[10]  A. Peeters,et al.  Global gyrokinetic simulations of intrinsic rotation in ASDEX Upgrade Ohmic L-mode plasmas , 2018, 1801.10600.

[11]  R. Dux,et al.  Measurement of the complete core plasma flow across the LOC–SOC transition at ASDEX Upgrade , 2018 .

[12]  C. Angioni,et al.  Theory-based modeling of LOC–SOC transitions in ASDEX Upgrade , 2017 .

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

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

[15]  Motoki Nakata,et al.  Isotope Effects on Trapped-Electron-Mode Driven Turbulence and Zonal Flows in Helical and Tokamak Plasmas. , 2017, Physical review letters.

[16]  P. Hennequin,et al.  Explaining the isotope effect on heat transport in L-mode with the collisional electron-ion energy exchange , 2017 .

[17]  D. H. Na,et al.  Experimental observations and modelling of intrinsic rotation reversals in tokamaks , 2017, 1701.08095.

[18]  J. Contributors,et al.  Isotope effects on L-H threshold and confinement in tokamak plasmas , 2017 .

[19]  C. Marini Poloidal CX visible light plasma rotation diagnostics in TCV , 2017 .

[20]  J. Dong,et al.  Isotope effects of trapped electron modes in the presence of impurities in tokamak plasmas , 2016 .

[21]  J. Citrin,et al.  Discriminating the trapped electron modes contribution in density fluctuation spectra , 2015 .

[22]  Matthew Reinke,et al.  The effects of dilution on turbulence and transport in C-Mod ohmic plasmas and comparisons with gyrokinetic simulations , 2014 .

[23]  F. Ryter,et al.  Core intrinsic rotation behaviour in ASDEX Upgrade ohmic L-mode plasmas , 2014 .

[24]  A. Hubbard,et al.  Changes in core electron temperature fluctuations across the ohmic energy confinement transition in Alcator C-Mod plasmas , 2013 .

[25]  T. Hahm,et al.  Isotopic dependence of residual zonal flows , 2013 .

[26]  A. Krämer-Flecken,et al.  Isotope effect and multiscale physics in fusion plasmas. , 2013, Physical review letters.

[27]  Jeff M. Candy,et al.  Isotope mass and charge effects in tokamak plasmas , 2011 .

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

[29]  Frank Jenko,et al.  The global version of the gyrokinetic turbulence code GENE , 2011, J. Comput. Phys..

[30]  R. Churchill,et al.  Observations of core toroidal rotation reversals in Alcator C-Mod ohmic L-mode plasmas , 2011 .

[31]  O. Sauter,et al.  Experimental demonstration of an up-down asymmetry effect on intrinsic rotation in the TCV tokamak , 2010 .

[32]  A. Bortolon Plasma rotation and momentum transport studies in the TCV tokamak based on charge exchange spectroscopy measurements , 2009 .

[33]  J. Rice,et al.  Spontaneous core toroidal rotation in Alcator C-Mod L-mode, H-mode and ITB plasmas , 2008 .

[34]  O. Sauter,et al.  Spontaneous L-mode plasma rotation scaling in the TCV tokamak , 2008 .

[35]  B. Duval,et al.  Bulk plasma rotation in the TCV tokamak in the absence of external momentum input , 2007 .

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

[37]  J. Weiland,et al.  Plasma rotation and momentum transport studies at JET , 2006 .

[38]  F. Leuterer,et al.  Experimental study of trapped-electron-mode properties in tokamaks: threshold and stabilization by collisions. , 2005, Physical review letters.

[39]  F. Jenko,et al.  Relationship between density peaking, particle thermodiffusion, Ohmic confinement, and microinstabilities in ASDEX Upgrade L-mode plasmas , 2005 .

[40]  C. Lechte,et al.  ρs scaling of characteristic turbulent structures in the torsatron TJ-K , 2005 .

[41]  Ulrich Stroth A comparative study of transport in stellarators and tokamaks , 1998 .

[42]  A. Bondeson,et al.  The CHEASE code for toroidal MHD equilibria , 1996 .

[43]  W. Horton,et al.  Studies of impurity mode and ion temperature gradient mode in toroidal plasmas , 1995 .

[44]  W. Dorland,et al.  Isotope scaling and ηi mode with impurities in tokamak plasmas , 1994 .

[45]  C. Gil,et al.  Turbulence and energy confinement in TORE SUPRA Ohmic discharges , 1992 .

[46]  B. Duval,et al.  Behaviour of plasma rotation and radial electric field with density ramp rate in an ohmically heated tokamak , 1992 .

[47]  W. Tang,et al.  Anomalous thermal confinement in ohmically heated tokamaks , 1986 .

[48]  W. Tang Microinstability-based model for anomalous thermal confinement in tokamaks , 1986 .

[49]  R. V. Neidigh,et al.  Plasma confinement studies in the ISX-A tokamak , 1979 .