Characteristics of type I ELM energy and particle losses in existing devices and their extrapolation to ITER
By Alberto Loarte, G. Saibene, R. Sartori, D. Campbell, M. Becoulet, L. Horton, T. Eich, A. Herrmann, G. Matthews, N. Asakura and 7 more. 2003
521 citations recorded by the source corpus.
Subfields: Aerospace Engineering, Materials Chemistry, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/bcc35cdf6534ef793e0cc2132f819b6bf958f470
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In Materials Chemistry
In Nuclear and High Energy Physics
Citations in the corpus
- A model of ELM filament energy evolution due to parallel losses (2005, unknown): “The pedestal stored energy decays on the MHD timescale, τ MHD ∼ 200–300 µs, which is typically comparable to or larger than the sonic timescale (Loarte et al 2003, Becoulet et al 2003, Loarte et al 2004).”
- Edge stability and transport control with resonant magnetic perturbations in collisionless tokamak plasmas (2006, background): “On the basis of an extensive multi-machine ELM database, it is well known that the impulsive energy released during an ELM increases with decreasing electron pedestal collisionalit”
- The JOREK non-linear extended MHD code and applications to large-scale instabilities and their control in magnetically confined fusion plasmas (2020, background): “Unmitigated type-I edge localized modes (ELMs) [28, 169] cannot be tolerated in ITER at least in full current operation [170] and even ELM types associated with reduced energy losses from the plasma and lower transient heat loads to plasma facing components, are likely not acceptable for DEMO [171].”