High-accuracy characterization of the edge radial electric field at ASDEX Upgrade

The installation of a new poloidal charge exchange recombination spectroscopy (CXRS) diagnostic at ASDEX Upgrade (AUG) has enabled the determination of the radial electric field, Er, using the radial force balance of impurity ions. Er has been derived from charge exchange (CX) spectra measured on different impurity species, such as He2+, B5+, C6+ and Ne10+. The resulting Er profiles are found to be identical within the uncertainties regardless of the impurity species used, thus, demonstrating the validity of the diagnostic technique. The Er profile has been compared to the main ion pressure gradient term, which is found to be the dominant contribution at the plasma edge, thus, supporting that the Er well is created by the main ion species. The Er profile has been measured in different confinement regimes including L-, I- and H-mode. The depth of the Er well and the magnitude of the Er shear are correlated with the ion pressure at the pedestal top. The temporal evolution of the measured CX profiles and the resulting Er have been studied during an edge-localized mode (ELM) cycle. At the ELM crash, the Er minimum is less deep resulting in a reduction of the E???B shear. Within 2?ms after the ELM crash, the edge kinetic profiles have nearly recovered and the Er well is observed to recover simultaneously. In high density type-I ELM mitigated H-mode plasmas, obtained via externally applied magnetic perturbations (MPs) with toroidal mode number n?=?2, no clear effect on Er due to the MPs has been observed.

[1]  L. G. Eliseev,et al.  Sheared flows and transition to improved confinement regime in the TJ-II stellarator , 2009 .

[2]  Wade,et al.  Rotation characteristics of main ions and impurity ions in H-mode tokamak plasma. , 1994, Physical review letters.

[3]  A. Mlynek,et al.  Studies of edge localized mode mitigation with new active in-vessel saddle coils in ASDEX Upgrade , 2011 .

[4]  E. Poli,et al.  Interaction of Mean and Oscillating Plasma Flows across Confinement Mode Transitions , 2010 .

[5]  K. Burrell,et al.  Parametric dependence of the edge radial electric field in the DIII-D tokamak , 1998 .

[6]  J. Stober,et al.  H-mode power threshold and transition in ASDEX Upgrade , 1998 .

[7]  K. Behler,et al.  ASDEX upgrade MHD equilibria reconstruction on distributed workstations , 2000 .

[8]  J. Hobirk,et al.  Measurement of poloidal fl ow, radial electriceld and E B shearing rates at ASDEX Upgrade , 2001 .

[9]  W. Suttrop,et al.  Practical Limitations to Plasma Edge Electron Temperature Measurements by Radiometry of Electron Cyclotron Emission , 1996 .

[10]  M. C. Zarnstorff,et al.  POLOIDAL ROTATION IN TFTR REVERSED SHEAR PLASMAS , 1998 .

[11]  Jeffrey H. Harris,et al.  Edge localized mode control with an edge resonant magnetic perturbation , 2005 .

[12]  D. Desideri,et al.  Plasma Potential Well and Velocity Shear Layer at the Edge of Reversed Field Pinch Plasmas , 1997 .

[13]  R. Dux,et al.  High-resolution charge exchange measurements at ASDEX Upgrade. , 2012, The Review of scientific instruments.

[14]  J. Ferreira,et al.  Effect of resonant magnetic perturbations on COMPASS-C tokamak discharges , 1992 .

[15]  R. J. Fonck,et al.  Determination of plasma-ion velocity distribution via charge-exchange recombination spectroscopy , 1984 .

[16]  W. Kasparek,et al.  Design of a New Doppler Reflectometer Frontend for the ASDEX Upgrade Tokamak , 2011 .

[17]  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.

[18]  E. Wolfrum,et al.  Probabilistic Lithium beam data analysis , 2008 .

[19]  B. Wieland Investigations on radial electric fields in the edge transport barrier of H-mode discharges , 2011 .

[20]  B. Scott,et al.  Intermittent transport across the scrape-off layer: latest results from ASDEX Upgrade , 2013 .

[21]  F. Hinton,et al.  Theory of plasma transport in toroidal confinement systems , 1976 .

[22]  R. Andre,et al.  Comparison of poloidal velocity measurements to neoclassical theory on the National Spherical Torus Experimenta) , 2010 .

[23]  K. Itoh,et al.  REVIEW ARTICLE: The role of the electric field in confinement , 1996 .

[24]  S. Coda,et al.  Beyond paradigm: Turbulence, transport, and the origin of the radial electric field in low to high confinement mode transitions in the DIII-D tokamak , 1995 .

[25]  S. Saarelma,et al.  L–H transition and pedestal studies on MAST , 2011 .

[26]  The effect of the radial electric field on neoclassical flows in a tokamak pedestal , 2011 .

[27]  B. Kurzan,et al.  Edge and core Thomson scattering systems and their calibration on the ASDEX Upgrade tokamak. , 2011, The Review of scientific instruments.

[28]  K. H. Burrell,et al.  Effects of E×B velocity shear and magnetic shear on turbulence and transport in magnetic confinement devices , 1997 .

[29]  J. Schweinzer,et al.  Improved chopping of a lithium beam for plasma edge diagnostic at ASDEX Upgrade. , 2012, The Review of scientific instruments.

[30]  Experimental studies of electron transport , 2001 .

[31]  Helmi Malova,et al.  Quasiadiabatic dynamics of charged particles in a space plasma , 2013 .

[32]  V. Toigo,et al.  Design of in-vessel saddle coils for MHD control in ASDEX Upgrade , 2008 .

[33]  L. L. Lao,et al.  Confinement physics of H-mode discharges in DIII-D , 1989 .

[34]  G Sips,et al.  Design of a digital multiradian phase detector and its application in fusion plasma interferometry. , 2010, The Review of scientific instruments.

[35]  K. Burrell Tests of causality: Experimental evidence that sheared E×B flow alters turbulence and transport in tokamaks , 1999 .

[36]  R. Marchand,et al.  Finite element modelling of transport in a tokamak edge and divertor , 2002 .

[37]  Naoto Tsujii,et al.  I-mode: an H-mode energy confinement regime with L-mode particle transport in Alcator C-Mod , 2010 .

[38]  R. Dux,et al.  ELM flushing and impurity transport in the H-mode edge barrier in ASDEX Upgrade , 2011 .

[39]  W. Suttrop,et al.  Plasma rotation profile measurements using Doppler reflectometry , 2004 .

[40]  S. Wolfe,et al.  A new look at density limits in tokamaks , 1988 .

[41]  T. Tala,et al.  Evolution of the radial electric field in a JET H-mode plasma , 2008 .

[42]  Bill Scott,et al.  Doppler Reflectometry for the Investigation of Propagating Density Perturbations , 2001 .

[43]  Julien Fuchs,et al.  Compatibility of ITER scenarios with full tungsten wall in ASDEX Upgrade , 2009 .

[44]  R. Scannell,et al.  The structure, evolution and role of the radial edge electric field in H-mode and L-mode on MAST , 2008 .

[45]  J. Coenen,et al.  Charge exchange recombination spectroscopy on a diagnostic hydrogen beam—measuring impurity rotation and radial electric field at the tokamak TEXTOR , 2010 .

[46]  F. Ryter,et al.  L- to H-mode transitions at low density in ASDEX Upgrade , 2011 .

[47]  Coupling of turbulence and reflectometer simulation codes and comparison with experiment , 2002 .

[48]  R. Jaenicke,et al.  Confinement in W7-AS and the role of radial electric field and magnetic shear , 1997 .

[49]  F. Wagner,et al.  Regime of Improved Confinement and High Beta in Neutral-Beam-Heated Divertor Discharges of the ASDEX Tokamak , 1982 .

[50]  T. Osborne,et al.  Edge impurity dynamics during an edge-localized mode cycle on DIII-D , 2005 .

[51]  Martin Jakobi,et al.  Transport into and across the scrape-off layer in the ASDEX Upgrade divertor tokamak , 2002 .

[52]  K. H. Burrell,et al.  Flow shear induced fluctuation suppression in finite aspect ratio shaped tokamak plasma , 1995 .

[53]  Christopher Portier,et al.  Risk factors for childhood leukaemia. Discussion and summary. , 2008, Radiation protection dosimetry.

[54]  H. Zohm,et al.  Inter-ELM behaviour of the electron density and temperature pedestal in ASDEX Upgrade , 2010 .

[55]  H. Sanuki,et al.  Physical Mechanism Determining the Radial Electric Field and its Radial Structure in a Toroidal Plasma , 1994 .

[56]  R. Dux,et al.  Investigation of passive edge emission in charge exchange spectra at the ASDEX Upgrade tokamak , 2011 .

[57]  Y. Sakamoto,et al.  Spatio-temporal structure of the edge radial electric field during H-mode in JT-60U , 2011 .

[58]  U. Stroth,et al.  Scale-selective turbulence reduction in H-mode plasmas in the TJ-II stellarator , 2011 .

[59]  M E Fenstermacher,et al.  Suppression of large edge-localized modes in high-confinement DIII-D plasmas with a stochastic magnetic boundary. , 2004, Physical review letters.

[60]  M. Hirsch,et al.  Dynamics of poloidal flows and turbulence at the H-mode transition in W7-AS , 2004 .

[61]  J. Huba NRL: Plasma Formulary , 2004 .

[62]  Paul W. Terry,et al.  Influence of sheared poloidal rotation on edge turbulence , 1990 .

[63]  J. Rice,et al.  Edge radial electric field structure and its connections to H-mode confinement in Alcator C-Mod plasmas , 2009 .

[64]  H. Zohm Edge localized modes (ELMs) , 1996 .

[65]  R. Dux,et al.  Evidence for strong inversed shear of toroidal rotation at the edge-transport barrier in the ASDEX upgrade. , 2009, Physical review letters.

[66]  Analysis of temperature and density pedestal in a multi-machine database , 2013 .

[67]  H. Zohm,et al.  The radial electric field and its associated shear in the ASDEX Upgrade tokamak , 2006 .

[68]  R. Dux,et al.  Poloidal asymmetry of parallel rotation measured in ASDEX Upgrade , 2012 .

[69]  K. Ida,et al.  Measurements of poloidal rotation velocity using charge exchange spectroscopy in a large helical device , 2000 .

[70]  G. Staebler,et al.  Impurity-induced turbulence suppression and reduced transport in the DIII-D tokamak , 2000 .

[71]  A. Loarte,et al.  Assessment of erosion of the ITER divertor targets during type I ELMs , 2003 .