2007
DOI: 10.1134/s1063776107010153
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Charge screening in a plasma with an external ionization source

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Cited by 47 publications
(20 citation statements)
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“…The obtained expressions are similar to those derived recently by Filippov et al 54 The only difference is associated with the fact that electron absorption on the grain was retained in Ref. Both these screening lengths depend on the strength of plasma production.…”
Section: ͑11͒supporting
confidence: 85%
“…The obtained expressions are similar to those derived recently by Filippov et al 54 The only difference is associated with the fact that electron absorption on the grain was retained in Ref. Both these screening lengths depend on the strength of plasma production.…”
Section: ͑11͒supporting
confidence: 85%
“…28, provided sink ͑loss͒ of plasma on the test particle is neglected ͓see also Eqs. This result is identical to that given by Eqs.…”
Section: Limiting Casesmentioning
confidence: 99%
“…This causes a nonexponential screening of the electrical potential and, at long enough distances, the potential exhibits an inverse power-law scaling instead of the exponential one. [27][28][29] In this paper we single out the effects of plasma production and loss by neglecting plasma absorption on the test particle surface. [15][16][17][18] In strongly collisional plasmas the potential has a Coulomb-like ͑ϰr −1 ͒ asymptote.…”
Section: Introductionmentioning
confidence: 99%
“…Here, T e is the electron temperature and e is the elementary charge. [10][11][12] Recently, it has been shown that plasma ionization-loss processes also play an important role in determining the qualitative nature of the interaction potential between positively charged particles. The point is that the shape of the potential distribution and hence the corresponding interaction potential between charged grains are not fixed but depend considerably on surrounding complex plasma conditions.…”
Section: Introductionmentioning
confidence: 99%