1986
DOI: 10.1007/bf00919519
|View full text |Cite
|
Sign up to set email alerts
|

A study of the collisionless interaction of interpenetrating super-Alfv�n plasma flows

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1

Citation Types

0
13
0

Year Published

1999
1999
2022
2022

Publication Types

Select...
7

Relationship

0
7

Authors

Journals

citations
Cited by 19 publications
(13 citation statements)
references
References 5 publications
0
13
0
Order By: Relevance
“…As shown explicitly by Hewett et al, 19 this electric field in turn accelerates ambient ions that, from the resulting E Â B drift, begin moving radially in a quarter gyroperiod. As a result, in the radial direction the magnetic field impedes the piston ions while accelerating the ambient ions and steepening the leading edge of the magnetic compression pulse, as seen in previous experiments 5 and numerical simulations. 21 Anomalous collisionless couplings, 20 such as through the modified or ion-ion two-stream instabilities, are unlikely to be the main coupling mechanism since, because of finite beta effects, 22 they are either not excited under these experimental conditions or their growth times are longer than the ambient ion gyroperiod.…”
mentioning
confidence: 73%
See 1 more Smart Citation
“…As shown explicitly by Hewett et al, 19 this electric field in turn accelerates ambient ions that, from the resulting E Â B drift, begin moving radially in a quarter gyroperiod. As a result, in the radial direction the magnetic field impedes the piston ions while accelerating the ambient ions and steepening the leading edge of the magnetic compression pulse, as seen in previous experiments 5 and numerical simulations. 21 Anomalous collisionless couplings, 20 such as through the modified or ion-ion two-stream instabilities, are unlikely to be the main coupling mechanism since, because of finite beta effects, 22 they are either not excited under these experimental conditions or their growth times are longer than the ambient ion gyroperiod.…”
mentioning
confidence: 73%
“…2 Laboratory experiments in the 1960s succeeded in producing strictly perpendicular magnetized collisionless shocks in h-pinches, 3,4 while efforts in the 1980s achieved some success creating perpendicular shocks using lasers. 5 More recently, several authors [6][7][8][9] have demonstrated that through an appropriate scaling of key dimensionless parameters, one can simulate astrophysically relevant collisionless shocks in a laboratory setting using lasers, which has the advantages of affording greater flexibility and control over reproducibility and, where strict fidelity cannot be achieved, of helping to validate computational codes.…”
mentioning
confidence: 99%
“…They do produce some hydrodynamic effects, such as the Vishniac instability, 22 that may also develop in collisionless systems. Certain experiments in Russia are most relevant here, 23,24 because they did produce collisionless shocks. In these experiments, an expanding, laser-produced plasma drove a shock wave through a plasma produced by a theta pinch.…”
Section: Contextmentioning
confidence: 99%
“…6,7 As early as 1964 it was recognized that a laser delivering power densities above 10 10 W/cm 2 could efficiently produce hot plasmas with the bulk of the laser energy mainly deposited into ion kinetic energy. 8 Since then, major advances in laser technology have created a growing area of research utilizing laser-produced plasmas ͑lpp͒ for a broad range of fields, including fusion research, [9][10][11] simulation of exploding supernovae 12,13 and thin film deposition. 14 The experiment presented here centers on the use of a laser to generate rapidly expanding, dense plasmas embedded in a background plasma.…”
Section: Introductionmentioning
confidence: 99%