Rippled shock propagation in a laser-driven target at multimegabar pressures

N N. Acharya (Department of Mechanical Engineering, University of Rochester 1 , Rochester, New York 14627,) H H. Pantell (Laboratory for Laser Energetics, University of Rochester 2 , Rochester, New York 14623,) D D. N. Polsin (Department of Mechanical Engineering, University of Rochester 1 , Rochester, New York 14627,) J J. R. Rygg (Department of Mechanical Engineering, University of Rochester 1 , Rochester, New York 14627,) G G. W. Collins P P. M. Celliers (Lawrence Livermore National Laboratory 2 , 7000 East Ave., Livermore, California 94550,) R R. Betti (Laboratory for Laser Energetics, University of Rochester 1 , Rochester, New York 14623-1299,) A A. E. Gleason H H. Aluie (Department of Mechanical Engineering, University of Rochester 1 , Rochester, New York 14627,) J J. K. Shang (Department of Mechanical Engineering, University of Rochester 1 , Rochester, New York 14627,)

Abstract

The evolution of non-uniform shocks produced by modulated laser irradiation or surface perturbations is relevant to studies of inertial confinement fusion and material properties at high-energy-density conditions. We present results from an experiment conducted at the OMEGA EP laser facility, where a 300 GPa shock was driven into a fused silica sample with pre-fabricated single-mode surface modulations. Using time-resolved optical velocimetry, we captured the continuous evolution of rippled shock motion, enabling a comprehensive mapping of the spatial amplitude history from formation to phase reversal in a single experiment. Initially, the ablation-driven shock inherits a fraction of the surface modulation amplitude from the sample, which subsequently grows before decaying, ultimately leading to the flattening of the rippled shock and a phase reversal. We find that two-dimensional inviscid hydrodynamic simulation of the experiment is able to qualitatively capture many aspects of the rippled shock evolution but over-predicts the initial amplitude growth. This experimental platform, capable of accommodating varying ripple wavelengths, lays the groundwork for a potential viscometry method at extreme pressures, where viscous effects manifest as differences in shock flattening times between rippled shocks of two distinct wavelengths propagating through the sample.

Article Details

Volume / Issue Vol. 137, Issue 11
Published March 21, 2025
ISSN 0021-8979
Publisher American Institute of Physics

Journal Info

Journal of Applied Physics

American Institute of Physics

ISSN: 0021-8979 Physical Sciences

Authors (10)

N

N. Acharya

Department of Mechanical Engineering, University of Rochester 1 , Rochester, New York 14627,

H

H. Pantell

Laboratory for Laser Energetics, University of Rochester 2 , Rochester, New York 14623,

D

D. N. Polsin

Department of Mechanical Engineering, University of Rochester 1 , Rochester, New York 14627,

J

J. R. Rygg

Department of Mechanical Engineering, University of Rochester 1 , Rochester, New York 14627,

G

G. W. Collins

P

P. M. Celliers

Lawrence Livermore National Laboratory 2 , 7000 East Ave., Livermore, California 94550,

R

R. Betti

Laboratory for Laser Energetics, University of Rochester 1 , Rochester, New York 14623-1299,

A

A. E. Gleason

H

H. Aluie

Department of Mechanical Engineering, University of Rochester 1 , Rochester, New York 14627,

J

J. K. Shang

Department of Mechanical Engineering, University of Rochester 1 , Rochester, New York 14627,