Solitary magnetic perturbations at the ELM onset
RP Wenninger, H Zohm, JE Boom, A Burckhart, MG Dunne, R Dux, T Eich, R, Fischer, C Fuchs, M Garcia-Munoz, V Igochine, M Hoelzl, NC Luhmann Jr, T, Lunt, M Maraschek, HW Mueller, HK Park, PA Schneider, F Sommer, W Suttrop, E, Viezzer, the ASDEX Upgrade Team

TL;DR
This paper investigates solitary magnetic perturbations (SMPs) near the ELM onset in tokamak plasmas, revealing their characteristics, origin, and potential role in understanding the non-linear phase of ELMs, which impact plasma confinement and material limits.
Contribution
It identifies SMPs as signatures of the non-linear ELM phase, providing insights into their origin, behavior, and relation to filament propagation, advancing understanding of ELM dynamics.
Findings
SMPs are field-aligned, rotating structures near ELM onset.
Number of peaks per toroidal turn is 1 or 2, lower than linear predictions.
SMPs correlate with the transition to filament propagation.
Abstract
Edge localised modes (ELMs) allow maintaining sufficient purity of tokamak H-mode plasmas and thus enable stationary H-mode. On the other hand in a future device ELMs may cause divertor power flux densities far in excess of tolerable material limits. The size of the energy loss per ELM is determined by saturation effects in the non-linear phase of the ELM, which at present is hardly understood. Solitary magnetic perturbations (SMPs) are identified as dominant features in the radial magnetic fluctuations below 100kHz. They are typically observed close (+-0.1ms) to the onset of pedestal erosion. SMPs are field aligned structures rotating in the electron diamagnetic drift direction with perpendicular velocities of about 10km/s. A comparison of perpendicular velocities suggests that the perturbation evoking SMPs is located at or inside the separatrix. Analysis of very pronounced examples…
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