1995
DOI: 10.1103/physreve.52.919
|View full text |Cite
|
Sign up to set email alerts
|

Heavy-ion interaction in a nonisothermal plasma with two-ion correlation effects

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1

Citation Types

0
3
0

Year Published

1996
1996
2018
2018

Publication Types

Select...
6

Relationship

0
6

Authors

Journals

citations
Cited by 8 publications
(3 citation statements)
references
References 12 publications
0
3
0
Order By: Relevance
“…(13), we have induced a cut-off wave number k max ¼ m e ðv 2 þ 2v 2 T Þ=ðZ 1 eÞ 2 to avoid the divergence of the integral caused by incorrect treatment of the short-range interactions between the projectile and electrons in the plasma. 23 Actually, the integral is fast convergent as increasing the values of the upper limit k max if the internuclear distance r keeps a limited value.…”
Section: Interaction Potentialmentioning
confidence: 99%
“…(13), we have induced a cut-off wave number k max ¼ m e ðv 2 þ 2v 2 T Þ=ðZ 1 eÞ 2 to avoid the divergence of the integral caused by incorrect treatment of the short-range interactions between the projectile and electrons in the plasma. 23 Actually, the integral is fast convergent as increasing the values of the upper limit k max if the internuclear distance r keeps a limited value.…”
Section: Interaction Potentialmentioning
confidence: 99%
“…where r = r(ρ, z) is the relative position vector, r = 2 is a cutoff wave number, which can avoid the divergence of the integral due to the wrong treatment of the short-range interactions between the projectile and the electrons in plasma. ρ η is the bound-electron charge density for a heavy ion in classical plasma [12,13] :…”
Section: Vicinage Effects In Coulomb Explosionmentioning
confidence: 99%
“…(1) where r = r(ρ, z) is the relative position vector, r = ρ 2 + z 2 , k max = m e (v 2 + 2v 2 T )/(Z 1 e) 2 is a cutoff wave number, which can avoid the divergence of the integral due to the wrong treatment of the short-range interactions between the projectile and the electrons in plasma. ρ η is the bound-electron charge density for a heavy ion in classical plasma [12,13] : ε(k, ω) shown in the interaction potential is the longitudinal dielectric function of the classical electron plasma, and can be expressed by:…”
Section: Vicinage Effects In Coulomb Explosionmentioning
confidence: 99%