2001
DOI: 10.1238/physica.regular.063a00194
|View full text |Cite
|
Sign up to set email alerts
|

Stopping Power in Semiclassical, Collisional Plasmas

Abstract: The stopping power in semiclassical plasmas with electron-ion collisions is evaluated. Collisional contribution is taken into account through an imaginary correction to the expression for the longitudinal dielectric function of collisionless plasmas. It is found that the collisions between charged particles result in enhancement of ion energy losses in the plasma medium. Results obtained are compared to data available from both experiments and computer simulation methods.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
16
0

Year Published

2001
2001
2018
2018

Publication Types

Select...
7

Relationship

0
7

Authors

Journals

citations
Cited by 17 publications
(16 citation statements)
references
References 15 publications
0
16
0
Order By: Relevance
“…The problem was thoroughly analyzed within the RPA [54,55,[61][62][63] and beyond by introducing an analytical formula for the LFC [54,[64][65][66][67], derived within the T -matrix approach [57,68], the method of effective potentials [69], or using the Mermin or more sophisticated models for the dielectric function [27] to name a few.…”
Section: Polarization Stopping Powermentioning
confidence: 99%
See 1 more Smart Citation
“…The problem was thoroughly analyzed within the RPA [54,55,[61][62][63] and beyond by introducing an analytical formula for the LFC [54,[64][65][66][67], derived within the T -matrix approach [57,68], the method of effective potentials [69], or using the Mermin or more sophisticated models for the dielectric function [27] to name a few.…”
Section: Polarization Stopping Powermentioning
confidence: 99%
“…(69) We observe that in the long-wavelength approximation, when ω 1 (k → 0) ω p , this expression (69) reduces to the generalized Drude-Lorentz model (19) if we choose Q 1 (k,w) = Q 1 (0,ω) = iν(ω) and that this model is unable to incorporate the asymptotic form (8), i.e., we have that −1 MM1 (k,w → ∞) 1 + ω 2 p /w 2 + · · · . Certainly, for a constant collision frequency or with Q 1 (k,w) = Q 1 (k,w = 0) = ih(k), h(k) > 0, the fact that the loss function L 1 (k,ω) = − Im −1 MM1 (k,ω)/ω has finite moments {C 0 (k),0,C 2 } can be easily checked by direct (analytic) integration.…”
Section: Three-moment Model Vs the Generalized Drude-lorentz Modelmentioning
confidence: 99%
“…is the effective electron-ion collision frequency [31]. The generalized Coulomb logarithm is given by [32] ln…”
Section: Local Field Correctionsmentioning
confidence: 99%
“…The dense plasma is formed in the experiments on heavy ion‐driven fusion, experiments at the National Ignition Facility, and magnetized Z‐pinch experiments . Currently, a large number of theoretical and experimental studies of physical processes that determine the design of the thermonuclear target are carried out. The study of energy losses of charged particles in the plasma is of great importance for dense plasma physics, as well as for solution of the problems of inertial fusion .…”
Section: Introductionmentioning
confidence: 99%