Dynamic measurement of impurity ion transport in runaway electron plateaus in DIII-D

E. M. Hollmann, A. Bortolon, F. Effenberg, N. Eidietis, D. Shiraki, I. Bykov, B. E. Chapman, J. Chen, S. Haskey, J. Herfindal, A. Lvovskiy, C. Marini, A. McLean, T. O'Gorman, M. D. Pandya, C. Paz-Soldan, Popović

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Abstract

The first dynamic (time-dependent) measurements of impurity ion radial (cross field) and parallel (along-field) diffusion coefficients for post-disruption runaway electron plateaus are presented. Small (∼1 mm diameter) carbon or silicon pellets are fired into the edge of steady-state runaway electron (RE) plateaus, and the resulting radial and toroidal transport of singly charged impurity ions (C+ or Si+) is monitored with spatially distributed visible spectrometers. Consistent with previous steady-state particle balance estimates of Ar+ radial transport, radial (cross field) diffusion coefficients D⊥ ≈ 2-5 m2/s are obtained, about 10 × larger than expected from neo-classical theory. Parallel diffusion coefficients D∥ ≈ 30-80 m2/s are estimated, also much (≈ 50 ×) larger than classical. It is speculated at present that these large diffusion coefficients may be due to turbulent transport. Indications of fairly significant (almost 2 ×) toroidal variation in electron density are seen in the RE plateaus, and this appears to cause some toroidal variation in impurity radial diffusion rates. Indications of slow (≈1 Hz) toroidal rotation in the impurity ions are observed, although the uncertainty in this measurement is large.

Original languageEnglish
Article number022503
JournalPhysics of Plasmas
Volume29
Issue number2
DOIs
StatePublished - Feb 1 2022

Funding

This work was supported in part by the U.S. Department of Energy under Contract Nos. DE-FG02-07ER54917, DE-FC02-04ER54698, DE-AC02-09CH11466, DE-AC05-00OR22725, DE-AC52-07NA27344, DE-FG02-04ER54744, and DE-AC05-06OR23100. The technical support of L. Chousal, J. Kulchar, and D. Ayala is gratefully acknowledged, as is diagnostic support of M. Austin, C. Chrystal, C. Lasnier, A. Moser, and M. Van Zeeland. Permission to use PrismSPECT from I. Golovkin is gratefully acknowledged.

FundersFunder number
U.S. Department of EnergyDE-AC05-00OR22725, DE-AC02-09CH11466, DE-FC02-04ER54698, DE-FG02-04ER54744, DE-AC52-07NA27344, DE-FG02-07ER54917, DE-AC05-06OR23100

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