Local measurements of the pedestal magnetic field profile throughout the ELM cycle on DIII-D

Author:

Burke M. G.1ORCID,Fonck R. J.2ORCID,McKee G. R.2ORCID,Burrell K. H.3ORCID,Haskey S. R.4ORCID,Knolker M.3ORCID,Laggner F. M.4ORCID,Osborne T. H.3,Victor B. S.1ORCID,Yan Z.2

Affiliation:

1. Lawrence Livermore National Laboratory, Livermore, California 94551, USA

2. University of Wisconsin, Madison, Wisconsin 53706, USA

3. General Atomics, San Diego, California 92121, USA

4. Princeton Plasma Physics Laboratory, Princeton, New Jersey 08540, USA

Abstract

New high speed localized measurements of the pedestal magnetic field during the edge localized mode (ELM) cycle of a DIII-D High confinement mode (H-mode) discharge indicate a temporally and spatial complex redistribution of the edge current density profile, jedge. The measurement technique extracts the magnetic field magnitude, B, via the spectral separation of Stark-split neutral beam radiation in the pedestal. Single spatial channel measurements from a novel spatial heterodyne spectrometer are validated in discharges with core current profile changes. The technique measures Stark-splitting changes that imply B changes as small as 1 mT with high time resolution (50  μs). At normalized poloidal flux [Formula: see text], B appears saturated in the inter-ELM period and then rapidly decreases in <200 μs by [Formula: see text], before edge recycling emission begins to increase. Radially inboard of jedge, B increases at the ELM crash. The behavior is consistent with a rapid collapse of jedge at the ELM crash and subsequent pedestal recovery. In some discharges, at [Formula: see text], changes in B are observed throughout the ELM cycle. In others, B recovers and is relatively stable until a few ms leading up to the next crash. Measurements of B during the H-mode transition show a large increase at [Formula: see text] with little change at [Formula: see text], consistent with the formation of the edge bootstrap current density peak. The [Formula: see text] spectrum is complicated by predicted changes to the Stark component intensities with density at the L–H transition.

Funder

U.S. Department of Energy

Publisher

AIP Publishing

Subject

Condensed Matter Physics

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