This page only displays the programme of the 45th European Physical Society Conference on Plasma Physics.
For more information go to https://eps2018.eli-beams.eu/
Chair: R. Dendy (live stream to Žofín Small Hall)
Chair: R. Dendy (live stream to Žofín Small Hall)
Chair: S. Coda (live stream to Žofín Small Hall)
Mánes Exhibition Hall: MCF P1.1x, BSAP P1.4x
Mánes Multifunctional Hall: BPIF P1.2x, LTDP P1.3x
Chair: R. Scott
Chair: M. Dieckmann
Chair: U. Cvelbar
Chair: X. Litaudon
Chair: C. Dougados
Chair: J. Berndt
Chair: J. Berndt
Chair: T. Grismayer
Chair: H. Thomas
Chair: E. Wolfrum
Chair: L. Frassinetti
Women in Plasma Physics Lunch
Mánes Exhibition Hall: MCF P2.1x, BSAP P2.4x
Mánes Multifunctional Hall: BPIF P2.2x, LTDP P2.3x
Physics of the Super H-Mode Regime: Record Performance on C-Mod and DIII-D, and Prospects for JET and ITER P.B. Snyder1, J.Hughes2, T. Osborne1, C. Paz-Soldan1, W. Solomon1, C-Mod/DIII-D teams 1 General Atomics, San Diego CA, USA 2 MIT PSFC, Cambridge MA, USA High fusion performance in tokamaks is enabled via the spontaneous formation of a transport barrier, or “pedestal.” While many open issues remain, progress in gyrokinetic, neoclassical and MHD theory and simulation [eg 1] has enabled a significant degree of predictive capability for the pedestal height and width, embodied in models such as EPED [2], which have been compared to hundreds of observations on several tokamaks (σ~0.25) [eg 2,3]. Notably, EPED predicts that, at very strong shaping, above a critical density, the pedestal solution bifurcates into multiple roots, including the usual H-mode pedestal root, and a “Super H-mode” (SH) root at very high pedestal pressure [Fig 1a]. Guided by predictions, the SH regime was discovered on DIII-D [4]. More recently, in the final two weeks of Alcator C-Mod operations, SH experiments achieved world record pedestal pressure (~80 kPa) [5], finding, as predicted, ITER-like pedestal pressure at ITER-like toroidal and poloidal field. New DIII-D SH experiments in 2017-18 have achieved high pedestals [Fig 1a] and fusion performance [Fig 1b], including what appears to be the highest QDD (and QDT_equiv~0.5) ever achieved on a medium scale tokamak (R<2m). Sustained high performance operation at low and high separatrix density has been achieved, using 3D magnetic perturbations to control density and achieve stationary profiles. Normalized metrics of fusion performance such as Q/IaB, or
W/PheatIaB, reach very high values in SH [Fig 1b]. Achieving similar levels of normalized performance could allow Q>1 in JET, or Q=10 in ITER at currents below 15MA. However, there are many challenges in achieving such performance, including methods for sustainment, impurity and ELM control, and compatibility of high triangularity shapes with nearby metal walls. We present SH theory compared to results on C-Mod and DIII-D, and predictions and challenges for SH on JET, ITER , JT-60SA and DEMO concepts. Access to High Performance Super H-Mode Regime on DIII-D 35 Pedestal Pressure [2*pe,ped, kPa] 30 t=2.4s 25 t=2.2s 20 15 t=1.9s 10 H-Mode 5 Near Super H Super H 0 3 4 5 6 7 8 9 10 11 12 Pedestal Density [ne,ped(Zeff/2)1/2,1019m-3] Figure 1: (a) Recent DIII-D experiments have achieved very high pedestal pressure, deep into the SH regime, simultaneously achieving high fusion performance. (b) A simple metric of normalized fusion performance (
W/PhIaB) illustrates the fusion benefit of Super H (solid symbols are existing data from cases with
> 50kPa). Approximate required values of this metric for various levels of ITER performance are also shown. [1] G.T.A. Huysmans PPCF 47 (2005) B165; D. Dickinson et al. PPCF 53 (2011) 115010; S. Saarelma et al. PPCF 59 (2017) 064001. [2] P.B. Snyder et al NF 51 (2011) 103016; PoP 16 (2009) 056118. [3] M.N.A. Beurskens et al NF 54 (2014) 043001; R.J. Groebner et al NF 53 (2013) 093024; M.G. Dunne et al PPCF 59 (2016) 025010; M. Komm et al NF 57 (2017) 056041. [4] W. Solomon et al PRL 113 (2014) 135001; P.B. Snyder et al NF 55 (2015) 083026. [5] J.W. Hughes 2018 to appear in Nucl. Fusion. Acknowledgment: Supported by the US DOE under DE-FG02-95ER54309, FC02-06ER54873, DE-FC02-04ER54698, DE-FC02-99ER54512.
</Chair: O. Klimo
Chair: T. Carter
Chair: A. Granier
Chair: G. Huijsmans
Chair: C. Michaut
Chair: J. Faure
Chair: M. Koepke
Chair: A. Dinklage
Chair: G. Pautasso
Chair: M. Mantsinen
Chair: S. Kar
Chair: E. Falize
Chair: A. Laricchiuta
Chair: J. Mailloux
Mánes Exhibition Hall: MCF P4.1x, BSAP P4.4x
Mánes Multifunctional Hall: BPIF P4.2x, LTDP P4.3x
Chair: A. Ravasio
Chair: M. Romé
Chair: J.-S. Yoon
Chair: T. Eich
Chair: B. Duval
T. Bell
Chair: M. Nakatsutsumi
Chair: E. Solano
Chair: V. Guerra
Chair: G. Ericsson
Mánes Exhibition Hall: MCF P5.1x, BSAP P5.4x
Mánes Multifunctional Hall: BPIF P5.2x, LTDP P5.3x
Chair: C. Riconda
Itoh prize, Ph.D. poster prizes
Chair: R. Dendy