Results 1 to 10 of about 120,584 (295)

Tungsten core accumulation study in EAST plasma with lower tungsten divertor by kinetic impurity transport model

open access: yesNuclear Materials and Energy, 2022
Tungsten (W) impurity transport and the corresponding core W accumulation is a critical issue in tokamak with W as plasma facing material. In this work, a kinetic W impurity transport code based on the guiding center approximation is applied for the ...
Yihan Wu   +5 more
doaj   +3 more sources

On neoclassical impurity transport in stellarator geometry [PDF]

open access: yesPlasma Physics and Controlled Fusion, 2013
The impurity dynamics in stellarators has become an issue of moderate concern due to the inherent tendency of the impurities to accumulate in the core when the neoclassical ambipolar radial electric field points radially inwards (ion root regime).
Beidler C D   +14 more
core   +4 more sources

Topological transport of mobile impurities [PDF]

open access: yesPhysical Review B, 2021
We study the Hall response of topologically trivial mobile impurities (Fermi polarons) interacting weakly with majority fermions forming a Chern-insulator background. This setting involves a rich interplay between the genuine many-body character of the polaron problem and the topological nature of the surrounding cloud.
Pimenov, D.   +5 more
openaire   +6 more sources

Suppression of anomalous impurity transport in NBI-heated W7-X plasmas

open access: yesNuclear Fusion, 2023
Radial impurity density profiles in two Wendelstein 7-X (W7-X) experiments heated by neutral beam injection (NBI) are analyzed with respect to their impurity transport properties.
T. Romba   +6 more
doaj   +1 more source

Enhancement of neoclassical impurity density up/down asymmetry and Pfirsch–Schlüter transport due to the plasma elongation in the tokamak plasmas

open access: yesNuclear Fusion, 2023
The standard neoclassical theory of the impurity transport in tokamak plasma is improved by including the plasma elongation effect. The neoclassical up/down asymmetry of the impurity density is largely enhanced by the plasma elongation and is under ...
Chengkang Pan
doaj   +1 more source

Pfirsch–Schlüter impurity transport in stellarators [PDF]

open access: yesPhysics of Plasmas, 2010
The Pfirsch–Schluter transport of impurities is calculated for stellarator geometry. Contrary to the tokamak case, where the only contribution to the particle flux arises from friction between different species, in a stellarator there is another source of impurity transport due to pressure anisotropy.
Braun, S., Helander, P.
openaire   +3 more sources

Observation of tearing mode triggering by sawtooth crash with high-Z impurity accumulation in EAST

open access: yesAIP Advances, 2023
The high-Z impurity accumulation in the plasma core could degrade the plasma performance and may affect sawtooth crash and trigger tearing modes (TMs) in experimental advanced superconducting tokamak (EAST).
Shanshan Pan   +11 more
doaj   +1 more source

Quantitative comparison of impurity transport in turbulence reduced and enhanced scenarios at Wendelstein 7-X

open access: yesNuclear Fusion, 2023
We assess the turbulent particle transport being responsible for the limitation of the confinement and, thus, the overall performance of the neoclassically optimized stellarator Wendelstein 7-X.
J.A. Alcusón   +15 more
doaj   +1 more source

OEDGE modeling of far-SOL tungsten impurity sources and screening in WEST

open access: yesNuclear Materials and Energy, 2022
The plasma background and impurity transport in the scrape-off layer (SOL) of the WEST tokamak are modeled for three discharges over a Psep power scan ranging between 1.5 and 2.35 MW. An extended modeling grid is used to investigate far-SOL sourcing from
J.B. Maeker   +10 more
doaj   +1 more source

Impurity and Trace Tritium Transport in Tokamak Edge Turbulence [PDF]

open access: yes, 2004
The turbulent transport of impurity or minority species, as for example Tritium, is investigated in drift-Alfv\'en edge turbulence. The full effects of perpendicular and parallel convection are kept for the impurity species. The impurity density develops
M. E. Perry   +3 more
core   +1 more source

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