1999
DOI: 10.1088/0741-3335/41/3/002
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Stochastic (E×B) diffusion of ions in a spatially periodical potential field

Abstract: This paper discusses the stochastic (E × B) motion of ions in the homogeneous magnetic field and in the spatially periodical electrostatic potential. This approach is used for the simulation of ion diffusion in potential structures formed at the boundary plasma in tokamaks. We show that the ion motion in such structures scales with a single dimensionless parameter R, which is a combination of amplitude and dimension of potential structures, magnetic field intensity and ion charge/mass ratio. The presented resu… Show more

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Cited by 10 publications
(13 citation statements)
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“…Considering a particle travelling on the hill, there appear, namely, two regimes of its motion. According to paper of Bellan [11] and of our paper [1], there appears an instability for the case with R ≥ 0.25. A particle with this parameter spirals downhill until it enters the separatrix region.…”
Section: Introductionmentioning
confidence: 68%
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“…Considering a particle travelling on the hill, there appear, namely, two regimes of its motion. According to paper of Bellan [11] and of our paper [1], there appears an instability for the case with R ≥ 0.25. A particle with this parameter spirals downhill until it enters the separatrix region.…”
Section: Introductionmentioning
confidence: 68%
“…To understand more properly to the effect of anomalous diffusion of ions, found in the regime of edge tokamak plasma turbulence, we have recently [1,2] started with very simple model of the turbulent potential. Instead of obviously time and spatially uncorrelated dependencies, we use the spatially periodical model shown in Figs.…”
Section: Introductionmentioning
confidence: 99%
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“…Some examples of this kind of studies are [2][3][4][5][6][7][8][9][10][11][12][13][14]. However, in principle other forms for Λ are possible.…”
Section: Introductionmentioning
confidence: 99%
“…There we used a very simplified model of the turbulent potential structures, namely a spatially periodic and time-independent potential. Using a Hamiltonian approach (which takes into account the cyclotron motion), we have found, for impurity ions C + and usual potential amplitudes, a substantial increase in the diffusion of these ions (both of the Gaussian and Lévy-walk forms) [4], resulting in the generation of a radial electric field [3]. Using a drift approximation for this case, no diffusion and no electric field is observed.…”
mentioning
confidence: 99%