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Short-pulse laser absorption via heating in ultrahigh intensity laser plasma interaction
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10.1063/1.2372463
/content/aip/journal/pop/13/11/10.1063/1.2372463
http://aip.metastore.ingenta.com/content/aip/journal/pop/13/11/10.1063/1.2372463
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

The density in the effective vacuum-plasma interface as a function of the normalized laser amplitude for different scale lengths.

Image of FIG. 2.
FIG. 2.

The critical laser amplitude as a function of the density scale length. In the domain labeled “II” there is no resonance to occur since .

Image of FIG. 3.
FIG. 3.

(a) The normalized vector potential and the electron density and (b) the normalized electrostatic field. Parameters are and .

Image of FIG. 4.
FIG. 4.

The power absorption as a function of the normalized laser amplitude for different scale lengths. The solid line is for , the dashed line for , and the dashed-dotted line for .

Image of FIG. 5.
FIG. 5.

(a) The normalized vector potential and the electron density and (b) the normalized electrostatic field. Parameters are and .

Image of FIG. 6.
FIG. 6.

The position of the absorption layer as a function of the laser amplitude for . The solid line is for and the dashed line for .

Image of FIG. 7.
FIG. 7.

The power absorption as a function of the normalized laser amplitude for different scale lengths. The solid line is for , the dashed line is for , and the dashed-dotted line for .

Image of FIG. 8.
FIG. 8.

The power absorption as a function of the scale length for .

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/content/aip/journal/pop/13/11/10.1063/1.2372463
2006-11-10
2014-04-16
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Short-pulse laser absorption via J×B heating in ultrahigh intensity laser plasma interaction
http://aip.metastore.ingenta.com/content/aip/journal/pop/13/11/10.1063/1.2372463
10.1063/1.2372463
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