Results 211 to 220 of about 127,246 (266)

Edge Plasma Control by LHD

open access: yesEdge Plasma Control by LHD
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Plasma Edge Turbulence

Physical Review Letters, 1983
Model mode-coupling equations for the resistive drift-wave instability are derived and numerically solved to study the properties of turbulence near a plasma edge. The wavenumber spectrum of the turbulence is found to exhibit an inverse cascade to form an isotropic, two-dimensional Kolmogorov spectrum, ${k}^{\ensuremath{-}3}$, in the large-wave-number ...
Akira Hasegawa, Masahiro Wakatani
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Plasma Edge Physics with B2‐Eirene

Contributions to Plasma Physics, 2006
AbstractThe B2‐Eirene code package was developed to give better insight into the physics in the scrape‐off layer (SOL), which is defined as the region of open field‐lines intersecting walls. The SOL is characterised by the competition of parallel and perpendicular transport defining by this a 2D system.
Schneider, R.   +7 more
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Ion Transport in Turbulent Edge Plasmas

Physical Review Letters, 1996
Edge plasmas, such as the tokamak scrape-off layer, exist as a consequence of a balance between cross-field diffusion and parallel losses. The former is usually anomalous, and is widely thought to be driven by strong electrostatic turbulence. It is shown that the anomalous diffusion affects the parallel ion transport by giving rise to a new type of ...
, Helander, , Hazeltine, , Catto
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Plasma Edge in Bi2Te3

Journal of Applied Physics, 1963
The reflectance minima associated with the free carrier plasma edges in p- and n-type Bi2Te3 have been observed at 78° and 300°K. The data together with the measured Hall and Seebeck coefficients have yielded combined band structure-relaxation time parameters when proper account is taken of the anisotropy.
Robert Sehr, Louis R. Testardi
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Plasma Edge Cooling During rf Heating.

Physical Review Letters, 1978
A new approach to prevent the influx of high-$Z$ impurities into the core of a tokamak discharge by using rf power to modify the edge plasma temperature profile is discussed. This concept is based on spectroscopic measurements on PLT (Princeton Large Torus) during ohmic heating and ATC (Adiabatic Toroidal Compressor) during rf heating.
S. Suckewer, R. J. Hawryluk
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