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Effects of Si admixture in a laser-produced Fe plasma
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View: Figures


Image of FIG. 1.
FIG. 1.

Comparison of the time-resolved ion currents per surface unit emitted by Fe and Si plasmas produced by KrF and Nd:YAG laser beams having of 23 and 3.5 ns, respectively. The scales were recalculated to a distance of 1 m from the target.

Image of FIG. 2.
FIG. 2.

Dependencies of the total charge states per unit of solid angle (left axis) and of the ratio of their charge (right axis) on the fluence of Nd:YAG (a) and KrF (b) laser beams focused on the pure Fe target, and Si one.

Image of FIG. 3.
FIG. 3.

Comparison of the total charge of ions emitted form Si plasma in rescaled fluences: the fluence of the KrF excimer laser, , was rescaled to the Nd:YAG laser fluence using the formula which takes into account the wavelength and the pulse duration of both the lasers.

Image of FIG. 4.
FIG. 4.

Reconstructed time-resolved abundances of ionized species with the use of the CEA at the distance of 1.9 m from the target. The target was irradiated by Nd:YAG laser pulses with fluence.

Image of FIG. 5.
FIG. 5.

Dependencies of the soft x-ray emission from Fe and Si plasmas and of their ratio on the Nd:YAG laser fluence.


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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Effects of 2 mass % Si admixture in a laser-produced Fe plasma