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Plasma Phys. Control. Fusion 53 (2011) 093001<br />
Topical Review<br />
Figure 42. A 3D simulation <strong>of</strong> a 16 mm diameter array <strong>of</strong> 16 × 15 µm Al wires driven by <strong>the</strong><br />
MAGPIE generator. The (red) surface <strong>of</strong> constant density equal to 0.1 kg m −3 is representative <strong>of</strong><br />
<strong>the</strong> <strong>dense</strong> plasma region, while <strong>the</strong> (green) surface at 0.003 kg m −3 is representative <strong>of</strong> <strong>the</strong> coronal<br />
plasma. On <strong>the</strong> right are contours <strong>of</strong> ln ρ in a slice through <strong>the</strong> x–z plane [324].<br />
shown in figure 42 have demonstrated much agreement with this interpretation <strong>of</strong> <strong>the</strong> data. It<br />
should be noted that <strong>the</strong> snowplough implosion is far less susceptible to RT instabilities. The<br />
main x-ray pulse occurs at stagnation <strong>of</strong> <strong>the</strong> snowplough implosion compressing <strong>the</strong> precursor<br />
plasma. Cuneo et al [323] have shown in detail that high current implosions on Z also agree<br />
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