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Group velocity dispersion and relativistic effects on the wakefield induced by chirped laser pulse in parabolic plasma channel
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10.1063/1.4798530
/content/aip/journal/pop/20/4/10.1063/1.4798530
http://aip.metastore.ingenta.com/content/aip/journal/pop/20/4/10.1063/1.4798530
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

(a) Variation of normalized on-axis intensity versus at (bold line) and at , for positive chirp ( ), negative chirp ( ), and un-chirped pulses ( ). (b) Time duration, (c) spot size, and (d) chirp parameter of laser pulse as afunction of for (bold line), (dashed-dotted line), and (dashed line). The laser and plasma initial parameters are and .

Image of FIG. 2.
FIG. 2.

(a) The normalized on-axis axial wake field (Ez ) at and (b) the normalized maximum radial wake field (Er ) at . (bold line), (dashed-dotted line), and (dashed line). The other simulation parameters are the same as in Fig. 1 .

Image of FIG. 3.
FIG. 3.

2-D evolution of (a) Ez and (b) Er as a function of and at . The other simulation parameters are the same as in Fig. 1 .

Image of FIG. 4.
FIG. 4.

Variation of on-axis electron density perturbation ( ) as a function of for (bold line), (dashed-dotted line), and (dashed line) at . The other simulation parameters are the same as in Fig. 1 .

Image of FIG. 5.
FIG. 5.

The axial wake-field as a function of initial intensity of laser pulse (a) in the presence of both relativistic and GVD effects and (b) in the absence of GVD effect at .

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/content/aip/journal/pop/20/4/10.1063/1.4798530
2013-04-03
2014-04-19
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Group velocity dispersion and relativistic effects on the wakefield induced by chirped laser pulse in parabolic plasma channel
http://aip.metastore.ingenta.com/content/aip/journal/pop/20/4/10.1063/1.4798530
10.1063/1.4798530
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