2002
DOI: 10.1103/physreve.65.045401
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Perturbation transfer from the front to rear surface of laser-irradiated targets

Abstract: We present experimental results on the perturbation transfer of laser irradiated planar foils. Perturbed polystyrene foils were irradiated directly by laser at intensity of 6 x 10(13) W/cm(2). We measured perturbations on the foils by side-on x-ray backlighting technique. Perturbations on the rear surface due to the rippled shock front were observed just after the shock breakout. We also observed feed-through of perturbations on the laser-irradiated surface that grows due to the Rayleigh-Taylor instability.

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Cited by 6 publications
(4 citation statements)
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“…An upwind space-time conservation elements/solution elements (CE/SE) scheme is used with second-order accuracy in both space and time (Shen et al 2015a;Shen, Wen & Zhang 2015b;Shen & Wen 2016). A volume-fraction-based five-equation model (Abgrall 1996;Shyue 1998) is used to illustrate the different species residing on both sides of the inhomogeneous interface. The contact discontinuity restoring Harten-Lax-van Leer contact Riemann solver (Toro, Spruce & Speares 1994) is used to determine the numerical fluxes between the conservation elements.…”
Section: Numerical Schemementioning
confidence: 99%
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“…An upwind space-time conservation elements/solution elements (CE/SE) scheme is used with second-order accuracy in both space and time (Shen et al 2015a;Shen, Wen & Zhang 2015b;Shen & Wen 2016). A volume-fraction-based five-equation model (Abgrall 1996;Shyue 1998) is used to illustrate the different species residing on both sides of the inhomogeneous interface. The contact discontinuity restoring Harten-Lax-van Leer contact Riemann solver (Toro, Spruce & Speares 1994) is used to determine the numerical fluxes between the conservation elements.…”
Section: Numerical Schemementioning
confidence: 99%
“…In the ICF, the disturbance at the hotspot–fuel interface originates from its initial perturbation, the feedthrough of the perturbation on the ablation surface and the driven inhomogeneity (Hsing & Hoffman 1997; Weir, Chandler & Goodwin 1998; Shigemori et al. 2002; Regan et al. 2004; Haan et al.…”
Section: Introductionmentioning
confidence: 99%
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“…However, ablative RTI is inevitable as a result of nonuniformities such as initial target surface roughness. These perturbations will then feed through in deeper layers of the D-T capsule, 12,13 seeding converging classical RTI at the pusher-fuel interface. 14,15 This will eventually degrade the symmetry of implosion and cause pollution of the central hot spot.…”
Section: Introductionmentioning
confidence: 99%