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Radiation pressure acceleration of corrugated thin foils by Gaussian and super-Gaussian beams
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10.1063/1.3671957
/content/aip/journal/pop/19/1/10.1063/1.3671957
http://aip.metastore.ingenta.com/content/aip/journal/pop/19/1/10.1063/1.3671957
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

(Color online) Shape (r versus z) (a) and temporal evolution of maximum ion energy (b) of an initially planar plasma foil irradiated by Gaussian beam for T = 25 wavecycles when , R0 = 8 and a0 = 5. Shape (c) and temporal evolution of maximum ion energy (d) of plasma foil irradiated by super-Gaussian beam for the same parameters.

Image of FIG. 2.
FIG. 2.

(Color online) Shape (r versus z) of an initially rippled plasma foil of initial ripple amplitude D = 0.01 and wavenumber when irradiated by Gaussian (a, b, c) and super-Gaussian (d, e, f) beams for T = 3, 6, 10 wavecycles when , R0 = 8 and a0 = 5.

Image of FIG. 3.
FIG. 3.

(Color online) Shape (r versus z) of an initially rippled plasma foil of initial ripple amplitude D = 0.01, 0.02, 0.03 and wavenumber when irradiated by Gaussian (a, b, c) and super-Gaussian (d, e, f) beams for T = 9 wavecycles when , R0 = 8 and a0 = 5.

Image of FIG. 4.
FIG. 4.

(Color online) Shape (r versus z) of an initially rippled plasma foil of initial ripple amplitude D = 0.01 and wavenumber when irradiated by Gaussian (a, b, c) and super-Gaussian (d, e, f) beams for T = 9 wavecycles when , R0 = 8 and a0 = 5.

Image of FIG. 5.
FIG. 5.

(Color online) Variation of transmission coefficient of the laser beam with foil thickness for (a) , , and . (b) , , and .

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/content/aip/journal/pop/19/1/10.1063/1.3671957
2012-01-05
2014-04-18
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Radiation pressure acceleration of corrugated thin foils by Gaussian and super-Gaussian beams
http://aip.metastore.ingenta.com/content/aip/journal/pop/19/1/10.1063/1.3671957
10.1063/1.3671957
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