2004
DOI: 10.1016/j.physleta.2004.10.069
|View full text |Cite
|
Sign up to set email alerts
|

Effects of relativistic and channel focusing on an intense laser beam propagating in a plasma channel: variational analysis

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
8
0

Year Published

2006
2006
2021
2021

Publication Types

Select...
8

Relationship

0
8

Authors

Journals

citations
Cited by 20 publications
(8 citation statements)
references
References 20 publications
0
8
0
Order By: Relevance
“…Under the action of this force, electrons are expelled transversely away from regions of high laser intensity in the long pulse length limit and ponderomotive self-channeling emerges. Previous studies on ponderomotive self-channeling [39][40][41] in parabolic channels revealed a more complex parameter space than in [38]. After comparisons, it can be found that ponderomotive self-channeling can result in a parameter region for catastrophic focusing, and apparently decreases the traditional propagation domain in parameter space for a parabolic channel.…”
Section: Introductionmentioning
confidence: 88%
See 1 more Smart Citation
“…Under the action of this force, electrons are expelled transversely away from regions of high laser intensity in the long pulse length limit and ponderomotive self-channeling emerges. Previous studies on ponderomotive self-channeling [39][40][41] in parabolic channels revealed a more complex parameter space than in [38]. After comparisons, it can be found that ponderomotive self-channeling can result in a parameter region for catastrophic focusing, and apparently decreases the traditional propagation domain in parameter space for a parabolic channel.…”
Section: Introductionmentioning
confidence: 88%
“…Taking into account ponderomotive self-channeling and the weakly relativistic limit (|a| 2 = 1, where a is the normalized vector potential and its normalization is presented after equation (2)), an intense laser beam propagating in an underdense plasma (n/n c < 1, where n is the density of the underdense plasma and n c is the critical density) is described by the following two equations [40][41][42][43][44]:…”
Section: Basic Model and Evolution Equationsmentioning
confidence: 99%
“…(21) and numerically investigate the properties of the laser pulse evolution, there are two familiar approximation approaches to get some ordinary differential equations (ODEs) from the NLSE which is a partial differential equation (PDE). The first approach is the variational method [29][30][31] and the second one is the paraxial approximation approach. 2,[19][20][21] Both of these two approaches assume the NLSE has a solution…”
Section: Pulse Width Evolutionmentioning
confidence: 99%
“…(23) qualitatively, the pseudo-potential method will be introduced here, which is frequently used in articles researching solitary waves. 29,30 Equation (23) has a form like g 00 ðzÞ ¼ FðgðzÞÞ ¼ À dVðgðzÞÞ dgðzÞ , it is not difficult but a little bit tedious to get the pseudo-potential function…”
Section: Pulse Width Evolutionmentioning
confidence: 99%
“…Many papers have investigated these focusing effects in the uniform plasma or preformed channel cases. [14][15][16][17][18][19][20] It has been found that the spot size of an laser pulse can evolve along the propagating axis with constant, periodically focusing and defocusing oscillations, and catastrophic focusing. Further, Zhang et al has investigated the existence conditions of solitary waves in a parabolic plasma channel.…”
Section: Introductionmentioning
confidence: 99%