Perturbations that seed Rayleigh-Taylor (RT) instability in laser-driven targets form during the early-time period. This time includes a shock wave transit from the front to the rear surface of the target, and a rarefaction wave transit in the opposite direction. During this time interval, areal mass perturbations caused by all sources of non-uniformity (laser imprint, surface ripple) are expected to oscillate. The first direct experimental observations of the areal mass oscillations due to ablative Richtmyer-Meshkov (RM) instability and feedout followed by the RT growth of areal mass modulation are discussed. The experiments were made with 40 to 99 mm thick planar plastic targets rippled either on the front or on the rear with a sine wave ...
Rayleigh–Taylor instability, the main source of symmetry degradation in ICF experiments, is seeded a...
The primary goals of this report are to (1) understand experimental radiography better (radiograph k...
The mass ablation rate has been measured using the 12-beam GEKKO XII glass laser. An X-ray pinhole c...
Eight beams carrying a shaped pulse from the NOVA laser were focused into a hohlraum with a total en...
The feedout process transfers mass perturbations from the rear to the front surface of a driven targ...
We report on results of an experimental study of the Richtmyer- Meshkov instability. The growth of t...
A series of elementary experiments on the hydrodynamic instability in the inertial confinement fusio...
Experiments have been conducted using the Nova laser system to investigate the growth of the Richtmy...
The Richtmyer-Meshkov instability (RMI) is experimentally investigated using several different initi...
Laser induced Richtmyer-Meshkov (RM) instabilities have previously been described. In particular, th...
The Richtmyer-Meshkov instability after reshock is investigated in shock tube experiments at the Wis...
Abstract. Rayleigh–Taylor instability, the main source of symmetry degradation in ICF experiments, i...
International audienceWhen a shock wave of several tens of GPa breaks out at a free surface, a mater...
A model experiment of magnetic field amplification (MFA) via the Richtmyer-Meshkov instability (RMI)...
Growth of hydrodynamic instabilities at the interfaces of inertial confinement fusion capsules (ICF)...
Rayleigh–Taylor instability, the main source of symmetry degradation in ICF experiments, is seeded a...
The primary goals of this report are to (1) understand experimental radiography better (radiograph k...
The mass ablation rate has been measured using the 12-beam GEKKO XII glass laser. An X-ray pinhole c...
Eight beams carrying a shaped pulse from the NOVA laser were focused into a hohlraum with a total en...
The feedout process transfers mass perturbations from the rear to the front surface of a driven targ...
We report on results of an experimental study of the Richtmyer- Meshkov instability. The growth of t...
A series of elementary experiments on the hydrodynamic instability in the inertial confinement fusio...
Experiments have been conducted using the Nova laser system to investigate the growth of the Richtmy...
The Richtmyer-Meshkov instability (RMI) is experimentally investigated using several different initi...
Laser induced Richtmyer-Meshkov (RM) instabilities have previously been described. In particular, th...
The Richtmyer-Meshkov instability after reshock is investigated in shock tube experiments at the Wis...
Abstract. Rayleigh–Taylor instability, the main source of symmetry degradation in ICF experiments, i...
International audienceWhen a shock wave of several tens of GPa breaks out at a free surface, a mater...
A model experiment of magnetic field amplification (MFA) via the Richtmyer-Meshkov instability (RMI)...
Growth of hydrodynamic instabilities at the interfaces of inertial confinement fusion capsules (ICF)...
Rayleigh–Taylor instability, the main source of symmetry degradation in ICF experiments, is seeded a...
The primary goals of this report are to (1) understand experimental radiography better (radiograph k...
The mass ablation rate has been measured using the 12-beam GEKKO XII glass laser. An X-ray pinhole c...