Jul 2 – 6, 2018
Žofín Palace
Europe/Prague timezone

P4.1064 Threshold Effect In Tearing Mode Stabilization

Jul 5, 2018, 2:00 PM
2h
Mánes

Mánes

Speaker

Nathaniel Joseph Fisch

Description

See the full Abstract at http://ocs.ciemat.es/EPS2018ABS/pdf/P4.1064.pdf Conferenceonon Plasma Plasma Physics, Physics 2018, Prague, Czech Republic P4.1064 Synchrotron spectra, images, and polarization measurements from runaway electrons in the Alcator C-Mod tokamak R.A. Tinguely1, R.S. Granetz1, M. Hoppe2, O. Embréus2, and T. Fülöp2 1 Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, USA 2 Department of Physics, Chalmers University of Technology, Göteborg, Sweden In the high-field, compact Alcator C-Mod tokamak, relativistic runaway electrons (REs) generated during flattop plasma discharges emit synchrotron radiation in the visible wavelength range. Thus, spectrometers, cameras, and the Motional Stark Effect diagnostic installed on C-Mod measure absolutely-calibrated spectra, distortion-corrected images, and polarization information, respectively, of REs throughout the plasma. Due to the complex interplay of the RE phase-space distribution, plasma magnetic topology, and detector geometry, the synthetic diagnostic SOFT [1] is used to simulate all three measurements and compare theory with experiment. As inputs, the RE momenta and density distributions are calculated using both a test-particle model [2 – 4] and kinetic solver CODE [5]. In particular, this work explores the following: (1) Synchrotron spectra observed from REs generated at three magnetic fields (B0 = 2.7, 5.4, and 7.8 T) indicate a decrease in RE energy as synchrotron power loss is enhanced at higher fields [6]. (2) Transport and MHD activity are incorporated into the analysis of synchrotron images to better explain interesting spatiotemporal features. (3) Profiles of linearly-polarized synchrotron emission intensity and polarization angle are explored as a novel diagnostic of RE dynamics. [1] M. Hoppe, et al., Nucl. Fusion 58 (2018). [2] J.R. Martín-Solís, et al., Phys. Plasmas 5 (1998). [3] J.W. Connor and R.J. Hastie, Nucl. Fusion 15 (1975). [4] M.N. Rosenbluth and S.V. Putvinski, Nucl. Fusion 37 (1997). [5] M. Landreman, et al., Comput. Phys. Commun. 185 (2014). [6] R.A. Tinguely, et al., submitted to Nucl. Fusion (2018). This work is supported by the US DOE (grant DE-FC02-99ER54512), using Alcator C-Mod, a DOE Office of Science User Facility; Vetenskapsrådet (Dnr 2014-5510); and the European Research Council (ERC-2014-CoG grant 647121).

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