D. W. Larson
Lawrence Livermore National Laboratory
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Featured researches published by D. W. Larson.
Review of Scientific Instruments | 2010
J. L. Kline; K. Widmann; A. Warrick; R.E. Olson; C. A. Thomas; A. S. Moore; L. J. Suter; O. L. Landen; D. A. Callahan; S. Azevedo; J. Liebman; S. H. Glenzer; A. D. Conder; S. Dixit; P. Torres; V. Tran; E. L. Dewald; J. Kamperschroer; L. J. Atherton; R. Beeler; L. V. Berzins; J. Celeste; C. A. Haynam; W. W. Hsing; D. W. Larson; B. J. MacGowan; D. E. Hinkel; D. H. Kalantar; R. L. Kauffman; J. D. Kilkenny
The first 96 and 192 beam vacuum Hohlraum target experiments have been fielded at the National Ignition Facility demonstrating radiation temperatures up to 340 eV and fluxes of 20 TW/sr as viewed by DANTE representing an ∼20 times flux increase over NOVA/Omega scale Hohlraums. The vacuum Hohlraums were irradiated with 2 ns square laser pulses with energies between 150 and 635 kJ. They produced nearly Planckian spectra with about 30±10% more flux than predicted by the preshot radiation hydrodynamic simulations. To validate these results, careful verification of all component calibrations, cable deconvolution, and software analysis routines has been conducted. In addition, a half Hohlraum experiment was conducted using a single 2 ns long axial quad with an irradiance of ∼2×10(15) W/cm(2) for comparison with NIF Early Light experiments completed in 2004. We have also completed a conversion efficiency test using a 128-beam nearly uniformly illuminated gold sphere with intensities kept low (at 1×10(14) W/cm(2) over 5 ns) to avoid sensitivity to modeling uncertainties for nonlocal heat conduction and nonlinear absorption mechanisms, to compare with similar intensity, 3 ns OMEGA sphere results. The 2004 and 2009 NIF half-Hohlraums agreed to 10% in flux, but more importantly, the 2006 OMEGA Au Sphere, the 2009 NIF Au sphere, and the calculated Au conversion efficiency agree to ±5% in flux, which is estimated to be the absolute calibration accuracy of the DANTEs. Hence we conclude that the 30±10% higher than expected radiation fluxes from the 96 and 192 beam vacuum Hohlraums are attributable to differences in physics of the larger Hohlraums.
Physics of Plasmas | 2013
J. L. Kline; D. A. Callahan; S. H. Glenzer; N. B. Meezan; J. D. Moody; D. E. Hinkel; O. S. Jones; A. J. Mackinnon; R. Bennedetti; R. L. Berger; D. K. Bradley; E. L. Dewald; I. Bass; C. Bennett; M. W. Bowers; G. K. Brunton; J. Bude; S. C. Burkhart; A. Condor; J. M. Di Nicola; P. Di Nicola; S. N. Dixit; T. Doeppner; E. G. Dzenitis; G. V. Erbert; J. Folta; G. P. Grim; S. Glenn; Alex V. Hamza; S. W. Haan
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.
Physics of Plasmas | 2013
C. Niemann; W. Gekelman; C. G. Constantin; E. T. Everson; D. B. Schaeffer; S. E. Clark; Dan Winske; A. Zylstra; Patrick Pribyl; Shreekrishna Tripathi; D. W. Larson; S. H. Glenzer; A. S. Bondarenko
The dynamics of an exploding laser-produced plasma in a large ambient magneto-plasma was investigated with magnetic flux probes and Langmuir probes. Debris-ions expanding at super-Alfvenic velocity (up to MA=1.5) expel the ambient magnetic field, creating a large (>20 cm) diamagnetic cavity. We observe a field compression of up to B/B0=1.5 as well as localized electron heating at the edge of the bubble. Two-dimensional hybrid simulations reproduce these measurements well and show that the majority of the ambient ions are energized by the magnetic piston and swept outside the bubble volume. Nonlinear shear-Alfven waves (δB/B0>25%) are radiated from the cavity with a coupling efficiency of 70% from magnetic energy in the bubble to the wave.
Fusion Science and Technology | 2016
M. Spaeth; K. R. Manes; D. H. Kalantar; P. Miller; J. Heebner; E. S. Bliss; D. R. Spec; T. Parham; Pamela K. Whitman; Paul J. Wegner; P. A. Baisden; J. Menapace; M. W. Bowers; S. J. Cohen; T. Suratwala; J. M. Di Nicola; M. A. Newton; J. J. Adams; J. B. Trenholme; R. G. Finucane; R. E. Bonanno; D. C. Rardin; P. A. Arnold; S. N. Dixit; G. V. Erbert; A. C. Erlandson; J. Fair; E. Feigenbaum; W. H. Gourdin; R. Hawley
Abstract The possibility of imploding small capsules to produce mini-fusion explosions was explored soon after the first thermonuclear explosions in the early 1950s. Various technologies have been pursued to achieve the focused power and energy required for laboratory-scale fusion. Each technology has its own challenges. For example, electron and ion beams can deliver the large amounts of energy but must contend with Coulomb repulsion forces that make focusing these beams a daunting challenge. The demonstration of the first laser in 1960 provided a new option. Energy from laser beams can be focused and deposited within a small volume; the challenge became whether a practical laser system can be constructed that delivers the power and energy required while meeting all other demands for achieving a high-density, symmetric implosion. The National Ignition Facility (NIF) is the laser designed and built to meet the challenges for study of high-energy-density physics and inertial confinement fusion (ICF) implosions. This paper describes the architecture, systems, and subsystems of NIF. It describes how they partner with each other to meet these new, complex demands and describes how laser science and technology were woven together to bring NIF into reality.
Fusion Science and Technology | 2016
E. I. Moses; J. D. Lindl; M. Spaeth; R. Patterson; Richard H. Sawicki; L. J. Atherton; P. A. Baisden; L J Lagin; D. W. Larson; B. J. MacGowan; G. H. Miller; D. C. Rardin; V. S. Roberts; B. M. Van Wonterghem; Paul J. Wegner
Abstract The National Ignition Facility (NIF) at Lawrence Livermore National Laboratory has been operational since March 2009 and has been transitioning to a user facility supporting ignition science, high energy density stockpile science, national security applications, and fundamental science. The facility has achieved its design goal of 1.8 MJ and 500 TW of 3ω light on target, and has performed target experiments with 1.9 MJ at peak powers of 410 TW. The National Ignition Campaign (NIC), established by the U.S. National Nuclear Security Administration in 2005, was responsible for transitioning NIF from a construction project to a national user facility. Besides the operation and optimization of the use of the NIF laser, the NIC program was responsible for developing capabilities including target fabrication facilities; cryogenic layering capabilities; over 60 optical, X-ray, and nuclear diagnostic systems; experimental platforms; and a wide range of other NIF facility infrastructure. This paper provides a summary of some of the key experimental results for NIF to date, an overview of the NIF facility capabilities, and the challenges that were met in achieving these capabilities. They are covered in more detail in the papers that follow.
Proceedings of SPIE | 2004
D. W. Larson
The National Ignition Facility (NIF) is designed with its high-value optical systems in cassettes called line-replaceable Units (LRUs). Virtually all of NIFs active components are assembled in one of approximately 4000 electrical and optical LRUs that serve between two and eight of NIFs 192 laser beamlines. Many of these LRUs are optomechanical assemblies that are roughly the size of a telephone booth. The primary design challenges for this hardware include meeting stringent mechanical precision, stability, and cleanliness requirements. Pre-production units of each LRU type have been fielded on the first bundle of NIF and have been used to demonstrate that NIF meets its performance objectives. This presentation provides an overview of NIF LRUs-and their design and production plans for building out the remaining NIF bundles.
2. annual solid state lasers for applications to inertial confinement fusion (ICF), Paris (France), 22-25 Oct 1996 | 1997
Mark Newton; D. W. Larson; J. M. Wilson; H. C. Harjes; M. E. Savage; R. L. Anderson
The National Ignition Facility (NIF) is a high energy glass laser system and target chamber that will be used for research in inertial confinement fusion. The 192 beams of the NIF laser system are pumped by over 8600 Xenon flashlamps. The power conditioning system for NIF must deliver nearly 300 MJ of energy to the flashlamps in a cost effective and reliable manner. The present system design has over 200 capacitive energy storage modules that store approximately 1.7 MJ each and deliver that energy through a single switch assembly to 20 parallel sets of two series flashlamps. Although these are many possible system designs, few will meet the aggressive cost goals necessary to make the system affordable. Sandia National Laboratory and Lawrence Livermore National Laboratory are developing the system and component technologies that will be required to build the power conditioning system for the National Ignition Facility. This paper will describe the ongoing development activities for the NIF power conditioning system.
Journal of Physics: Conference Series | 2016
E. I. Moses; J. Atherton; L J Lagin; D. W. Larson; C. Keane; B. J. MacGowan; R. Patterson; M. Spaeth; B. Van Wonterghem; Paul J. Wegner; R. L. Kauffman
The National Ignition Facility (NIF) at Lawrence Livermore National Laboratory (LLNL) has been operational since March 2009 and has been transitioning to a user facility supporting ignition science, high energy density science (HEDS), national security applications, and fundamental science. The facility has achieved its design goal of 1.8 MJ and 500 TW of 3ω light on target, and has performed target experiments with 1.9 MJ at peak powers of 410 TW. The facility is on track to perform over 200 target shots this year in support of all of its user communities. The facility has nearly 60 diagnostic systems operational and has shown flexibility in laser pulse shape and performance to meet the requirements of its multiple users. Progress continues on its goal of demonstrating thermonuclear burn in the laboratory. It has performed over 40 indirect-drive experiments with cryogenic-layered capsules. New platforms are being developed for HEDS and fundamental science. Equation-of-state and material strength experiments have been done on a number of materials with pressures of over 50 MBars obtained in diamond, conditions never previously encountered in the laboratory and similar to those found in planetary interiors. Experiments are also in progress investigating radiation transport, hydrodynamic instabilities, and direct drive implosions. NIF continues to develop as an experimental facility. Advanced Radiographic Capability (ARC) is now being installed on NIF for producing high-energy radiographs of the imploded cores of ignition targets and for short pulse laser-plasma interaction experiments. One NIF beam is planned for conversion to two picosecond beams in 2014. Other new diagnostics such as x-ray Thomson scattering, low energy neutron spectrometer, and multi-layer reflecting x-ray optics are also planned. Incremental improvements in laser performance such as improved optics damage performance, beam balance, and back reflection control are being pursued.
Proceedings of SPIE | 2017
M. W. Bowers; Jeff Wisoff; Mark Herrmann; Tom Anklam; Jay W. Dawson; Jean-Michel G Di Nicola; C. Haefner; Mark Hermann; D. W. Larson; Christopher D. Marshall; Bruno M. Van Wonterghem; Paul J. Wegner
This talk will provide an overview of high power laser research at Lawrence Livermore National Laboratory (LLNL). It will discuss the status of the National Ignition Facility (NIF) laser. In addition, the talk will describe other laser development activities such as the development of high average power lasers and novel fiber lasers. The National Ignition Facility (NIF) has been in service since 2007 and operating with > 1 MJ energies since 2009. During this time the facility has transitioned to become an international user facility and increased the shot rate from ~150 target shots per year to greater than 400 shots per year. Today, the NIF plays an essential role in the US Stockpile Stewardship Program, providing data under the extreme conditions needed to validate computer models and train the next generation of stockpile stewards. Recent upgrades include the Advanced Radiographic Capability (ARC), a high energy short pulse laser used to do high resolution radiography. In addition to the NIF, this talk will include an overview of progress on the high average power laser development, recent results from fiber laser development activities and improvements to laser design and computational capabilities.
Journal of Physics: Conference Series | 2016
B M Van Wonterghem; R. L. Kauffman; D. W. Larson; Mark Herrmann
Since its completion in 2009, the National Ignition Facility has been operated in support of NNSAs Stockpile Stewardship mission, providing unique experimental data in the high energy density regime. We will describe the progress made by the National Ignition facility in the user office and management, facility capabilities, target diagnostics and diagnostics development. We will also discuss the results of a major effort to increase the shot rate on NIF. An extensive set of projects, developed in conjunction with the HED community and drawing on best practices at other facilities, improved shot rate by over 80% and recently enabled us to deliver 356 target experiments in FY15 in support of the users. Through an updated experimental set-up and review process, computer controlled set-up of the laser and diagnostics and disciplined operations, NIF also continued to deliver experimental reliability, precision and repeatability. New and complex platforms are introduced with a high success rate. Finally we discuss how new capabilities and further efficiency improvements will enable the successful execution of ICF and HED experimental programs required to support the quest for Ignition and the broader Science Based Stockpile Stewardship mission