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Dive into the research topics where Bernhard H. Wilde is active.

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Featured researches published by Bernhard H. Wilde.


Physics of Plasmas | 1995

Design and modeling of ignition targets for the National Ignition Facility

S. W. Haan; Stephen M. Pollaine; J. D. Lindl; Laurance J. Suter; R. L. Berger; Linda V. Powers; W. Edward Alley; Peter A. Amendt; John A. H. Futterman; W. Kirk Levedahl; Mordecai D. Rosen; Dana P. Rowley; Richard A. Sacks; Aleksei I. Shestakov; George L. Strobel; Max Tabak; S. V. Weber; George B. Zimmerman; William J. Krauser; Douglas Wilson; Stephen V. Coggeshall; David B. Harris; Nelson M. Hoffman; Bernhard H. Wilde

Several targets are described that in simulations give yields of 1–30 MJ when indirectly driven by 0.9–2 MJ of 0.35 μm laser light. The article describes the targets, the modeling that was used to design them, and the modeling done to set specifications for the laser system in the proposed National Ignition Facility. Capsules with beryllium or polystyrene ablators are enclosed in gold hohlraums. All the designs utilize a cryogenic fuel layer; it is very difficult to achieve ignition at this scale with a noncryogenic capsule. It is necessary to use multiple bands of illumination in the hohlraum to achieve sufficiently uniform x‐ray irradiation, and to use a low‐Z gas fill in the hohlraum to reduce filling of the hohlraum with gold plasma. Critical issues are hohlraum design and optimization, Rayleigh–Taylor instability modeling, and laser–plasma interactions.


Physics of Plasmas | 1996

Ignition target design and robustness studies for the National Ignition Facility

William J. Krauser; Nelson M. Hoffman; Douglas Wilson; Bernhard H. Wilde; William S. Varnum; David B. Harris; Fritz J. Swenson; P. A. Bradley; S. W. Haan; Stephen M. Pollaine; A. S. Wan; J. C. Moreno; Peter A. Amendt

Recent results are presented from two‐dimensional LASNEX [G. B. Zimmerman and W. L. Kruer, Comments Plasmas Phys. Controlled Thermonucl. Fusion 2, 51 (1975)] calculations of the indirectly driven hohlraum and ignition capsules proposed for the National Ignition Facility (NIF). The calculations concentrate on two capsule designs, the baseline design that has a bromine‐doped plastic ablator, and the beryllium design that has a copper‐doped beryllium ablator. Both capsules have a cryogenic fuel layer. Primary emphasis in these calculations is placed upon robustness studies detailing various sensitivities. Because of computer modeling limitations these studies fall into two categories: those performed with integrated modeling where the capsule, hohlraum, and laser rays all are modeled simultaneously with the laser power levels as the only energy input; and those performed in a capsule‐only mode where an externally imposed radiative flux is applied to the exterior of the capsule, and only the capsule performan...


Physics of Plasmas | 2002

Supersonic jet and shock interactions

J. M. Foster; Bernhard H. Wilde; Paula A. Rosen; T.S. Perry; M. Fell; M. J. Edwards; Barbara F. Lasinski; R. E. Turner; M. L. Gittings

Supersonic fluid flow and the interaction of strong shock waves to produce jets of material are ubiquitous features of inertial confinement fusion (ICF), astrophysics, and other fields of high energy-density science. The availability of large laser systems provides an opportunity to investigate such hydrodynamic systems in the laboratory, and to test their modeling by radiation hydrocodes. We describe experiments to investigate the propagation of a structured shock front within a radiation-driven target assembly, the formation of a supersonic jet of material, and the subsequent interaction of this jet with an ambient medium in which a second, ablatively driven shock wave is propagating. The density distribution within the jet, the Kelvin–Helmholz roll-up at the tip of the jet, and the jet’s interaction with the counterpropagating shock are investigated by x-ray backlighting. The experiments were designed and modeled using radiation hydrocodes developed by Los Alamos National Laboratory, AWE, and Lawrence Livermore National Laboratory. The same hydrocodes are being used to model a large number of other ICF and high energy-density physics experiments. Excellent agreement between the different simulations and the experimental data is obtained, but only when the full geometry of the experiment, including both laser-heated hohlraum targets (driving the jet and counter-propagating shock), is included. The experiments were carried out at the University of Rochester’s Omega laser [J. M. Soures et al., Phys. Plasmas 3, 2108 (1996)].


Physics of Plasmas | 1998

Evidence of plasma fluctuations and their effect on the growth of stimulated Brillouin and stimulated Raman scattering in laser plasmas

D. S. Montgomery; B. B. Afeyan; James A. Cobble; Juan C. Fernandez; Mark D. Wilke; S. H. Glenzer; R. K. Kirkwood; B. J. MacGowan; J. D. Moody; E. L. Lindman; D. H. Munro; Bernhard H. Wilde; Harvey A. Rose; D. F. DuBois; B. Bezzerides; H. X. Vu

The reflectivity levels of stimulated Brillouin scattering (SBS) in recent large scale length laser plasma experiments is much lower than expected for conditions where the convective gain exponent is expected to be large. Long wavelength velocity fluctuations caused during the plasma formation process, or by parametric instabilities themselves, have been proposed as a mechanism to detune SBS in these experiments and reduce its gain. Evidence of large velocity fluctuation levels is found in the time-resolved SBS spectra from these experiments, and correlates with observed changes in the reflectivity of both SBS and stimulated Raman scattering (SRS). The authors present evidence of fluctuations which increase as the plasma density systematically increases, and discuss their effect on the growth of parametric instabilities.


Physics of Plasmas | 1996

Symmetry experiments in gas‐filled hohlraums at NOVA

Norman D. Delamater; T. J. Murphy; Allan A. Hauer; R. L. Kauffman; A. L. Richard; E. L. Lindman; Glenn Ronald Magelssen; Bernhard H. Wilde; David B. Harris; B. A. Failor; J. M. Wallace; L. V. Powers; Stephen M. Pollaine; L. J. Suter; R. E. Chrien; T. D. Shepard; Harvey A. Rose; E. A. Williams; M. B. Nelson; M. D. Cable; J. B. Moore; M. A. Salazar; K. Gifford

Understanding drive symmetry in gas‐filled hohlraums is currently of interest because the baseline design of the indirect drive ignition target for the planned National Ignition Facility uses a gas‐filled hohlraum. This paper reports on the results of a series of experiments performed at the Nova laser [C. Bibeau et al. Appl. Opt. 31, 5799 (1992)] facility at Lawrence Livermore National Laboratory with the goal of understanding time‐dependent drive symmetry in gas filled hohlraums. Time‐dependent symmetry data from capsule implosions and reemission targets in gas‐filled hohlraums are discussed. Results of symmetry measurements using thin wall gas‐filled hohlraums are also discussed. The results show that the gas is effective in impeding the motion of the wall blowoff material, and that the resulting implosion performance of the capsule is not significantly degraded from vacuum results. The implosion symmetry in gas differs from vacuum results with similar laser pointing indicating a shift in beam position...


The Astrophysical Journal | 2009

Laboratory Experiments, Numerical Simulations, and Astronomical Observations of Deflected Supersonic Jets: Application to HH 110

Patrick Hartigan; J. M. Foster; Bernhard H. Wilde; Robert Francis Coker; Paula A. Rosen; J. F. Hansen; B.E. Blue; R. J. R. Williams; R. Carver; Adam Frank

Collimated supersonic flows in laboratory experiments behave in a similar manner to astrophysical jets provided that radiation, viscosity, and thermal conductivity are unimportant in the laboratory jets and that the experimental and astrophysical jets share similar dimensionless parameters such as the Mach number and the ratio of the density between the jet and the ambient medium. When these conditions apply, laboratory jets provide a means to study their astrophysical counterparts for a variety of initial conditions, arbitrary viewing angles, and different times, attributes especially helpful for interpreting astronomical images where the viewing angle and initial conditions are fixed and the time domain is limited. Experiments are also a powerful way to test numerical fluid codes in a parameter range in which the codes must perform well. In this paper, we combine images from a series of laboratory experiments of deflected supersonic jets with numerical simulations and new spectral observations of an astrophysical example, the young stellar jet HH 110. The experiments provide key insights into how deflected jets evolve in three dimensions, particularly within working surfaces where multiple subsonic shells and filaments form, and along the interface where shocked jet material penetrates into and destroys the obstacle along its path. The experiments also underscore the importance of the viewing angle in determining what an observer will see. The simulations match the experiments so well that we can use the simulated velocity maps to compare the dynamics in the experiment with those implied by the astronomical spectra. The experiments support a model where the observed shock structures in HH 110 form as a result of a pulsed driving source rather than from weak shocks that may arise in the supersonic shear layer between the Mach disk and bow shock of the jets working surface.


Physics of Plasmas | 1995

Gas‐filled targets for large scale‐length plasma interaction experiments on Nova

L. V. Powers; R. L. Berger; R. L. Kauffman; B. J. MacGowan; Peter A. Amendt; C. A. Back; T. P. Bernat; S. Dixit; D. I. Eimerl; K. G. Estabrook; J. A. Harte; D. H. Kalantar; D. E. Klem; Barbara F. Lasinski; D. S. Montgomery; J. D. Moody; D. H. Munro; T. D. Shepard; L. J. Suter; R. E. Turner; E. A. Williams; Juan C. Fernandez; W. W. Hsing; Bernhard H. Wilde; B. H. Failor

Stimulated Brillouin backscatter from large scale‐length gas‐filled targets has been measured on the Nova laser. These targets were designed to approximate conditions in indirect drive ignition target designs in underdense plasma electron density (ne∼1021/cm3), temperature (Te≳3 keV), and gradient scale lengths (Ln∼2 mm, Lv≳6 mm) as well as calculated gain for stimulated Brillouin scattering (SBS). The targets used in these experiments were gas‐filled balloons with polyimide walls (gasbags) and gas‐filled hohlraums. Detailed characterization using x‐ray imaging and x‐ray and optical spectroscopy verifies that the calculated plasma conditions are achieved. Time‐resolved SBS backscatter from these targets is <3% for conditions similar to ignition target designs.


Physics of Plasmas | 1997

Measurements of laser-plasma instability relevant to ignition hohlraums

Juan C. Fernandez; Bruno S. Bauer; James A. Cobble; D. F. DuBois; George A. Kyrala; D. S. Montgomery; Harvey A. Rose; H. X. Vu; Robert G. Watt; Bernhard H. Wilde; Mark D. Wilke; William Monford Wood; B. H. Failor; R. K. Kirkwood; B. J. MacGowan

The potential for laser-plasma instability is a serious concern for indirect-drive inertial confinement fusion (ICF), where laser beams illuminate the interior of a cavity (called a hohlraum) to produce x-rays for imploding a fusion capsule symmetrically. The speckled nature of laser beams used in ICF is an important factor in laser-plasma instability processes. For example, models which calculate the spatial growth of convective instability by properly accounting for the laser speckles successfully predict the observed onsets of backscattering due to stimulated Brillouin and Raman scattering instabilities (SBS and SRS). Assuming pump depletion as the only saturation mechanism in these models results in very large predicted levels of SBS and SRS backscattering from the long-scale plasmas expected in ignition hohlraums. However, in the long-scale plasmas studied in the Nova and Trident lasers [E. M. Campbell, Rev. Sci. Instrum. 57, 2101 (1986) and N. K. Moncur et al., Appl. Opt. 34, 4274 (1995)], SRS and S...


Physics of Plasmas | 2005

Three-Dimensional Hydrodynamic Experiments on the National Ignition Facility

B. E. Blue; H. F. Robey; S. G. Glendinning; Matthew J. Bono; Scott C. Burkhart; J. Celeste; R. F. Coker; R. Costa; S. Dixit; J. M. Foster; J. F. Hansen; C. A. Haynam; Mark Hermann; J. P. Holder; W. W. Hsing; D. H. Kalantar; N. E. Lanier; D. A. Latray; H. Louis; B. J. MacGowan; G. R. Maggelssen; Christopher D. Marshall; E. I. Moses; A. J. Nikitin; D. W. O'Brien; T.S. Perry; M. W. Poole; V. V. Rekow; P.A. Rosen; M. B. Schneider

The production of supersonic jets of material via the interaction of a strong shock wave with a spatially localized density perturbation is a common feature of inertial confinement fusion and astrophysics. The behavior of two-dimensional (2D) supersonic jets has previously been investigated in detail [J. M. Foster et. al, Phys. Plasmas 9, 2251 (2002)]. In three-dimensions (3D), however, there are new aspects to the behavior of supersonic jets in compressible media. In this paper, the commissioning activities on the National Ignition Facility (NIF) [J. A. Paisner et al., Laser Focus World 30, 75 (1994)] to enable hydrodynamic experiments will be presented as well as the results from the first series of hydrodynamic experiments. In these experiments, two of the first four beams of NIF are used to drive a 40 Mbar shock wave into millimeter scale aluminum targets backed by 100 mg/cc carbon aerogel foam. The remaining beams are delayed in time and are used to provide a point-projection x-ray backlighter source for diagnosing the three-dimensional structure of the jet evolution resulting from a variety of 2D and 3D features. Comparisons between data and simulations using several codes will be presented.


Review of Scientific Instruments | 1999

Measurement and simulation of apertures on Z hohlraums

R. E. Chrien; W. Matuska; George C. Idzorek; Fritz J. Swenson; D.L. Peterson; Bernhard H. Wilde; John L. Porter; Stephen P. Breeze; L. E. Ruggles; Walter W. Simpson; M. Vargas

We have performed aperture measurements and simulations for vacuum hohlraums heated by wire array implosions. A low-Z plastic coating is often applied to the aperture to create a high ablation pressure which retards the expansion of the gold hohlraum wall. However this interface is unstable and may be subject to the development of highly nonlinear perturbations (“jets”) as a result of shocks converging near the edge of the aperture. These experiments have been simulated using Lagrangian and Eulerian radiation hydrodynamics codes.

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Paula A. Rosen

Atomic Weapons Establishment

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J. M. Foster

University of Rochester

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T. S. Perry

Lawrence Livermore National Laboratory

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B. J. MacGowan

Lawrence Livermore National Laboratory

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Juan C. Fernandez

Los Alamos National Laboratory

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Robert Francis Coker

Los Alamos National Laboratory

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Adam Frank

University of Rochester

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R. E. Chrien

Los Alamos National Laboratory

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D. S. Montgomery

Los Alamos National Laboratory

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Harvey A. Rose

Los Alamos National Laboratory

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