2005
DOI: 10.1088/0963-0252/14/1/013
|View full text |Cite
|
Sign up to set email alerts
|

Theoretical modelling of an x-ray source based on stochastic acceleration of charged particles at electron cyclotron resonance

Abstract: The motion of charged particles in the field of H-waves of a cylindrical and a rectangular waveguide in the presence of a uniform magnetic field is investigated analytically and numerically. We obtain the equations of charged particle motion in the H-wave field under cyclotron resonance conditions, evaluate the width of nonlinear resonances, and establish the criterion for dynamical chaos emergence. The criterion is used to analyse the possibility of stochastic acceleration of charged particles by the field of… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
1
0

Year Published

2009
2009
2011
2011

Publication Types

Select...
2

Relationship

1
1

Authors

Journals

citations
Cited by 2 publications
(1 citation statement)
references
References 37 publications
0
1
0
Order By: Relevance
“…The analytical model of IEDFs in a single-frequency capacitive collisionless rf sheath gives only the qualitative features of IEDFs due to the approximations such as the constant sheath width and the sinusoidal sheath potential drop [1][2][3]. The IEDFs on the driven electrode are affected by the ratio of the ion transit time (τ ion ) to the rf period (τ rf ), which is expressed as functions of the rf frequency, the sheath length and the mean potential difference between the driven electrode and the plasma [1,[4][5][6]. When τ ion /τ rf 1, ions respond to the instantaneous sheath voltage.…”
Section: Introductionmentioning
confidence: 99%
“…The analytical model of IEDFs in a single-frequency capacitive collisionless rf sheath gives only the qualitative features of IEDFs due to the approximations such as the constant sheath width and the sinusoidal sheath potential drop [1][2][3]. The IEDFs on the driven electrode are affected by the ratio of the ion transit time (τ ion ) to the rf period (τ rf ), which is expressed as functions of the rf frequency, the sheath length and the mean potential difference between the driven electrode and the plasma [1,[4][5][6]. When τ ion /τ rf 1, ions respond to the instantaneous sheath voltage.…”
Section: Introductionmentioning
confidence: 99%