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H. Wilkens

Bio: H. Wilkens is an academic researcher from General Atomics. The author has contributed to research in topics: Hohlraum & Ignition system. The author has an hindex of 7, co-authored 7 publications receiving 853 citations.

Papers
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Journal ArticleDOI
TL;DR: Miller et al. as discussed by the authors proposed a point design for the initial ignition campaign on the National Ignition Facility (NIF) using D-T fusion fuel in an ablator of either CH with Ge doping, or Be with Cu.
Abstract: Point design targets have been specified for the initial ignition campaign on the National Ignition Facility [G. H. Miller, E. I. Moses, and C. R. Wuest, Opt. Eng. 443, 2841 (2004)]. The targets contain D-T fusion fuel in an ablator of either CH with Ge doping, or Be with Cu. These shells are imploded in a U or Au hohlraum with a peak radiation temperature set between 270 and 300 eV. Considerations determining the point design include laser-plasma interactions, hydrodynamic instabilities, laser operations, and target fabrication. Simulations were used to evaluate choices, and to define requirements and specifications. Simulation techniques and their experimental validation are summarized. Simulations were used to estimate the sensitivity of target performance to uncertainties and variations in experimental conditions. A formalism is described that evaluates margin for ignition, summarized in a parameter the Ignition Threshold Factor (ITF). Uncertainty and shot-to-shot variability in ITF are evaluated, and...

534 citations

Journal ArticleDOI
TL;DR: In this article, a detailed simulation-based model of the June 2011 National Ignition Campaign cryogenic DT experiments is presented, which is based on integrated hohlraum-capsule simulations that utilize the best available models for the HLS, ablator, and DT equations of state and opacities.
Abstract: A detailed simulation-based model of the June 2011 National Ignition Campaign cryogenic DT experiments is presented. The model is based on integrated hohlraum-capsule simulations that utilize the best available models for the hohlraum wall, ablator, and DT equations of state and opacities. The calculated radiation drive was adjusted by changing the input laser power to match the experimentally measured shock speeds, shock merger times, peak implosion velocity, and bangtime. The crossbeam energy transfer model was tuned to match the measured time-dependent symmetry. Mid-mode mix was included by directly modeling the ablator and ice surface perturbations up to mode 60. Simulated experimental values were extracted from the simulation and compared against the experiment. Although by design the model is able to reproduce the 1D in-flight implosion parameters and low-mode asymmetries, it is not able to accurately predict the measured and inferred stagnation properties and levels of mix. In particular, the measured yields were 15%–40% of the calculated yields, and the inferred stagnation pressure is about 3 times lower than simulated.

112 citations

Journal ArticleDOI
TL;DR: In this paper, a series of three symcap implosion experiments with nearly identical target, laser, and diagnostics configurations are reproducible at the level of ±8.5% absolute and ±2% relative, respectively.
Abstract: Indirect drive experiments have now been carried out with laser powers and energies up to 520 TW and 1.9 MJ. These experiments show that the energy coupling to the target is nearly constant at 84% ± 3% over a wide range of laser parameters from 350 to 520 TW and 1.2 to 1.9 MJ. Experiments at 520 TW with depleted uranium hohlraums achieve radiation temperatures of ∼330 ± 4 eV, enough to drive capsules 20 μm thicker than the ignition point design to velocities near the ignition goal of 370 km/s. A series of three symcap implosion experiments with nearly identical target, laser, and diagnostics configurations show the symmetry and drive are reproducible at the level of ±8.5% absolute and ±2% relative, respectively.

66 citations

Journal ArticleDOI
J. D. Lindl1, L. J. Atherton1, P.A. Amednt1, Steven H. Batha2, P. Bell1, Richard Berger1, Riccardo Betti3, D. L. Bleuel1, T. R. Boehly3, D. K. Bradley1, Dave Braun1, D. A. Callahan1, P. M. Celliers1, C. J. Cerjan1, Daniel S. Clark1, Gilbert Collins1, R.C. Cook1, E. L. Dewald1, Laurent Divol1, S. N. Dixit1, E. G. Dzenitis1, M. J. Edwards1, James E. Fair1, R. J. Fortner1, Johan Frenje4, V. Yu. Glebov3, Siegfried Glenzer1, Gary Grim2, S. W. Haan1, A. V. Hamza1, B. A. Hammel1, D. R. Harding3, S. P. Hatchett1, C. A. Haynam1, Hans W. Herrmann2, Mark Herrmann5, Damien Hicks1, D. E. Hinkel1, Darwin Ho1, Nelson M. Hoffman2, H. Huang6, Nobuhiko Izumi1, B. Jacoby1, O. S. Jones1, Daniel H. Kalantar1, Robert L. Kauffman1, J. D. Kilkenny6, R. K. Kirkwood1, John Kline2, J. P. Knauer3, J. A. Koch1, B. J. Kozioziemski1, G. A. Kyrala2, K. N. La Fortune1, O. L. Landen1, David Larson1, R. A. Lerche1, S. Le Pape1, R. A. London1, B. J. MacGowan1, A. J. Mackinnon1, T. N. Malsbury1, Evan Mapoles1, M. M. Marinak1, P. W. McKenty3, N. Meezan1, D. D. Meyerhofer3, Pierre Michel1, Jose Milovich1, John Moody1, Michael J. Moran1, K. A. Moreno6, Edward I. Moses1, D. H. Munro1, Abbas Nikroo6, R. E. Olson5, T. G. Parham1, R. W. Patterson1, Kyle Peterson5, R. D. Petrasso4, S. M. Pollaine1, Joseph Ralph1, Sean Regan3, Harry Robey1, M. D. Rosen1, R. A. Sacks1, Jay D. Salmonson1, T. C. Sangster3, S.M. Sepke1, D. H. Schneider1, Marilyn Schneider1, M. Shaw1, Brian Spears1, P. T. Springer1, Christian Stoeckl3, L. J. Suter1, Cliff Thomas1, R. Tommasini1, Richard Town1, B.M. VanWonterghem1, Roger Alan Vesey5, S. V. Weber1, Paul J. Wegner1, K. Widman1, C. Clay Widmayer1, M. Wilke2, H. Wilkens6, E. A. Williams1, Doug Wilson2, B. K. Young1 
TL;DR: The National Ignition Facility at Lawrence Livermore National Laboratory was formally dedicated in May 2009 and the hohlraum energetic series culminated with an experiment that irradiated an ignition scale HLS with 1 MJ as mentioned in this paper.
Abstract: The National Ignition Facility at Lawrence Livermore National Laboratory was formally dedicated in May 2009. The hohlraum energetics campaign with all 192 beams began shortly thereafter and ran until early December 2009. These experiments explored hohlraum-operating regimes in preparation for experiments with layered cryogenic targets. The hohlraum energetic series culminated with an experiment that irradiated an ignition scale hohlraum with 1 MJ. The results demonstrated the ability to produce a 285 eV radiation environment in an ignition scale hohlraum while meeting ignition requirements for symmetry, backscatter and hot electron production. Complementary scaling experiments indicate that with ~1.3 MJ, the capsule drive temperature will reach 300 eV, the point design temperature for the first ignition campaign. Preparation for cryo-layered implosions included installation of a variety of nuclear diagnostics, cryogenic layering target positioner, advanced optics and facility modifications needed for tritium operations and for routine operation at laser energy greater than 1.3 MJ. The first cyro-layered experiment was carried out on 29 September 2010. The main purpose of this shot was to demonstrate the ability to integrate all of the laser, target and diagnostic capability needed for a successful cryo-layered experiment. This paper discusses the ignition point design as well as findings and conclusions from the hohlraum energetics campaign carried out in 2009. It also provides a brief summary of the initial cryo-layered implosion.

54 citations


Cited by
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Journal ArticleDOI
20 Feb 2014-Nature
TL;DR: In this article, the authors report the achievement of fusion fuel gains exceeding unity on the US National Ignition Facility using a high-foot implosion method, which is a manipulation of the laser pulse shape in a way that reduces instability in the implosion.
Abstract: Ignition is needed to make fusion energy a viable alternative energy source, but has yet to be achieved. A key step on the way to ignition is to have the energy generated through fusion reactions in an inertially confined fusion plasma exceed the amount of energy deposited into the deuterium-tritium fusion fuel and hotspot during the implosion process, resulting in a fuel gain greater than unity. Here we report the achievement of fusion fuel gains exceeding unity on the US National Ignition Facility using a 'high-foot' implosion method, which is a manipulation of the laser pulse shape in a way that reduces instability in the implosion. These experiments show an order-of-magnitude improvement in yield performance over past deuterium-tritium implosion experiments. We also see a significant contribution to the yield from α-particle self-heating and evidence for the 'bootstrapping' required to accelerate the deuterium-tritium fusion burn to eventually 'run away' and ignite.

733 citations

Journal ArticleDOI
TL;DR: In this article, Zhou et al. presented the initial condition dependence of Rayleigh-Taylor (RT) and Richtmyer-Meshkov (RM) mixing layers, and introduced parameters that are used to evaluate the level of mixedness and mixed mass within the layers.

606 citations

Journal ArticleDOI
TL;DR: Miller et al. as discussed by the authors proposed a point design for the initial ignition campaign on the National Ignition Facility (NIF) using D-T fusion fuel in an ablator of either CH with Ge doping, or Be with Cu.
Abstract: Point design targets have been specified for the initial ignition campaign on the National Ignition Facility [G. H. Miller, E. I. Moses, and C. R. Wuest, Opt. Eng. 443, 2841 (2004)]. The targets contain D-T fusion fuel in an ablator of either CH with Ge doping, or Be with Cu. These shells are imploded in a U or Au hohlraum with a peak radiation temperature set between 270 and 300 eV. Considerations determining the point design include laser-plasma interactions, hydrodynamic instabilities, laser operations, and target fabrication. Simulations were used to evaluate choices, and to define requirements and specifications. Simulation techniques and their experimental validation are summarized. Simulations were used to estimate the sensitivity of target performance to uncertainties and variations in experimental conditions. A formalism is described that evaluates margin for ignition, summarized in a parameter the Ignition Threshold Factor (ITF). Uncertainty and shot-to-shot variability in ITF are evaluated, and...

534 citations

Journal ArticleDOI
TL;DR: The National Ignition Campaign (NIC) as mentioned in this paper was a multi-institution effort established under the National Nuclear Security Administration of DOE in 2005, prior to the completion of the NIF in 2009.
Abstract: The National Ignition Campaign (NIC) was a multi-institution effort established under the National Nuclear Security Administration of DOE in 2005, prior to the completion of the National Ignition Facility (NIF) in 2009. The scope of the NIC was the planning and preparation for and the execution of the first 3 yr of ignition experiments (through the end of September 2012) as well as the development, fielding, qualification, and integration of the wide range of capabilities required for ignition. Besides the operation and optimization of the use of NIF, these capabilities included over 50 optical, x-ray, and nuclear diagnostic systems, target fabrication facilities, experimental platforms, and a wide range of NIF facility infrastructure. The goal of ignition experiments on the NIF is to achieve, for the first time, ignition and thermonuclear burn in the laboratory via inertial confinement fusion and to develop a platform for ignition and high energy density applications on the NIF. The goal of the NIC was to develop and integrate all of the capabilities required for a precision ignition campaign and, if possible, to demonstrate ignition and gain by the end of FY12. The goal of achieving ignition can be divided into three main challenges. The first challenge is defining specifications for the target, laser, and diagnostics with the understanding that not all ignition physics is fully understood and not all material properties are known. The second challenge is designing experiments to systematically remove these uncertainties. The third challenge is translating these experimental results into metrics designed to determine how well the experimental implosions have performed relative to expectations and requirements and to advance those metrics toward the conditions required for ignition. This paper summarizes the approach taken to address these challenges, along with the progress achieved to date and the challenges that remain. At project completion in 2009, NIF lacked almost all the diagnostics and infrastructure required for ignition experiments. About half of the 3 yr period covered in this review was taken up by the effort required to install and performance qualify the equipment and experimental platforms needed for ignition experiments. Ignition on the NIF is a grand challenge undertaking and the results presented here represent a snapshot in time on the path toward that goal. The path forward presented at the end of this review summarizes plans for the Ignition Campaign on the NIF, which were adopted at the end of 2012, as well as some of the key results obtained since the end of the NIC.

509 citations

Journal ArticleDOI
TL;DR: A review of the current state of the art in inertial confinement fusion research can be found in this paper, where the authors describe the underlying physical principles of fusion energy production from controlled nuclear fusion reactions.
Abstract: The quest for controlled fusion energy has been ongoing for over a half century. The demonstration of ignition and energy gain from thermonuclear fuels in the laboratory has been a major goal of fusion research for decades. Thermonuclear ignition is widely considered a milestone in the development of fusion energy, as well as a major scientific achievement with important applications in national security and basic sciences. The US is arguably the world leader in the inertial confinement approach to fusion and has invested in large facilities to pursue it, with the objective of establishing the science related to the safety and reliability of the stockpile of nuclear weapons. Although significant progress has been made in recent years, major challenges still remain in the quest for thermonuclear ignition via laser fusion. Here, we review the current state of the art in inertial confinement fusion research and describe the underlying physical principles. The quest for energy production from controlled nuclear fusion reactions has been ongoing for many decades. Here, the inertial confinement fusion approach, based on heating and compressing a fuel pellet with intense lasers, is reviewed.

475 citations