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Perturbation evolution started by Richtmyer-Meshkov instability in planar laser targets
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10.1063/1.2227272
/content/aip/journal/pop/13/8/10.1063/1.2227272
http://aip.metastore.ingenta.com/content/aip/journal/pop/13/8/10.1063/1.2227272
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

(Color) (a) Theoretical time histories of for classical light-to-heavy RM instability: total (red line), and contribution to it due to the interfacial perturbation (blue line). (b) Simulated for a shock-interface interaction in an unbounded medium (solid line) and in a finite-thickness Nike target (dashed line). (c) Simulated density map for the classical RM case at the moment marked by the solid circle in (b); TS, RS, and MI denote transmitted and reflected shock fronts and material interface, respectively. (d) The same for the Nike target at the moment marked by the empty circle in (b).

Image of FIG. 2.
FIG. 2.

Simulated (black) and measured (gray lines) for a target irradiated from the foam side by Nike pulses without (a) and with a foot (b). Stars in (a), (b) indicate the onset of acceleration. (c) Lineouts of the streak records at 3 and showing a phase reversal of the areal mass modulation.

Image of FIG. 3.
FIG. 3.

Simulated (black) and measured (gray lines) for a target irradiated from the plastic side by Nike pulses without (a) and with a foot (b). Stars in (a), (b) indicate the onset of acceleration. Gray solid and dashed lineouts represent two shots taken consequently in order to cover whole laser pulse without a foot.

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/content/aip/journal/pop/13/8/10.1063/1.2227272
2006-08-24
2014-04-16
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Perturbation evolution started by Richtmyer-Meshkov instability in planar laser targets
http://aip.metastore.ingenta.com/content/aip/journal/pop/13/8/10.1063/1.2227272
10.1063/1.2227272
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