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Effect of laser light polarization on generation of relativistic ion beams driven by an ultraintense laser
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10.1063/1.4803709
/content/aip/journal/jap/113/17/10.1063/1.4803709
http://aip.metastore.ingenta.com/content/aip/journal/jap/113/17/10.1063/1.4803709
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

The mean energy of carbon ions (a) and protons (b) for the target thickness equal 1 m and both types of polarization. The mean energy of carbon ions obtained from the LS model is added to the plot (a) for a comparison.

Image of FIG. 2.
FIG. 2.

The electric field vector (E) along the axis of propagation of the laser beam and the charge density in the early stage of simulation for the 1 m target and the laser intensity equal to 10 W/cm for both types of polarization: circular (a) and linear (b).

Image of FIG. 3.
FIG. 3.

The charge density for 1 m target and the laser intensity equal to 10 W/cm for both types of polarization: linear (a) and circular (b).

Image of FIG. 4.
FIG. 4.

The energy conversion efficiency for carbon ions (a) and proton (b) for the target thickness equal to 1 m and both types of polarization.

Image of FIG. 5.
FIG. 5.

The standard ion energy deviation for carbon ions (a) and protons (b) for the target thickness equal to 1m and both types of polarization.

Image of FIG. 6.
FIG. 6.

The energy spectrum of carbon ions for the 1 m target, laser intensity equal to 10W/cm for CP and 2.0 × 10 W/cm for LP and both types of polarization.

Image of FIG. 7.
FIG. 7.

The energy spectrum of protons for the 1 m target, laser intensity equal to 10W/cm for CP and 2.0 × 10 W/cm for LP and both types of polarization.

Image of FIG. 8.
FIG. 8.

The mean energy of carbon ions (a) and protons (b) for the laser intensity equal to 10W/cm for CP and 2.0 × 10 W/cm for LP and both types of polarization. The mean energy of carbon ions obtained from the LS model is added to the plot (a) for a comparison.

Image of FIG. 9.
FIG. 9.

The charge density for the 0.1m target and the laser intensity equal to 10W/cm and linear polarization of the laser beam.

Image of FIG. 10.
FIG. 10.

The energy conversion efficiency for carbon ions (a) and protons (b) for the laser intensity equal to 10 W/cm for CP and 2.0 × 10 W/cm for LP and both types of polarization.

Image of FIG. 11.
FIG. 11.

The standard ion energy deviation for carbon ions (a) and protons (b) for the laser intensity equal to 10 W/cm for CP and 2.0 × 10 W/cm for LP and both types of polarization.

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/content/aip/journal/jap/113/17/10.1063/1.4803709
2013-05-07
2014-04-23
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Effect of laser light polarization on generation of relativistic ion beams driven by an ultraintense laser
http://aip.metastore.ingenta.com/content/aip/journal/jap/113/17/10.1063/1.4803709
10.1063/1.4803709
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