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Dive into the research topics where O. L. Landen is active.

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Featured researches published by O. L. Landen.


Physics of Plasmas | 2004

The physics basis for ignition using indirect-drive targets on the National Ignition Facility

J. D. Lindl; Peter A. Amendt; R. L. Berger; S. Gail Glendinning; S. H. Glenzer; S. W. Haan; R. L. Kauffman; O. L. Landen; L. J. Suter

The 1990 National Academy of Science final report of its review of the Inertial Confinement Fusion Program recommended completion of a series of target physics objectives on the 10-beam Nova laser at the Lawrence Livermore National Laboratory as the highest-priority prerequisite for proceeding with construction of an ignition-scale laser facility, now called the National Ignition Facility (NIF). These objectives were chosen to demonstrate that there was sufficient understanding of the physics of ignition targets that the laser requirements for laboratory ignition could be accurately specified. This research on Nova, as well as additional research on the Omega laser at the University of Rochester, is the subject of this review. The objectives of the U.S. indirect-drive target physics program have been to experimentally demonstrate and predictively model hohlraum characteristics, as well as capsule performance in targets that have been scaled in key physics variables from NIF targets. To address the hohlrau...


Physics of Plasmas | 2011

Point design targets, specifications, and requirements for the 2010 ignition campaign on the National Ignition Facility

S. W. Haan; J. D. Lindl; D. A. Callahan; D. S. Clark; J. D. Salmonson; B. A. Hammel; L. J. Atherton; R. Cook; M. J. Edwards; S. H. Glenzer; Alex V. Hamza; S. P. Hatchett; Mark Herrmann; D. E. Hinkel; D. Ho; H. Huang; O. S. Jones; J. L. Kline; G. A. Kyrala; O. L. Landen; B. J. MacGowan; M. M. Marinak; D. D. Meyerhofer; J. L. Milovich; K. A. Moreno; E. I. Moses; David H. Munro; A. Nikroo; R. E. Olson; Kyle Peterson

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...


Physics of Plasmas | 2014

Review of the National Ignition Campaign 2009-2012

J. D. Lindl; O. L. Landen; John Edwards; Ed Moses

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.


Science | 2010

Symmetric Inertial Confinement Fusion Implosions at Ultra-High Laser Energies

S. H. Glenzer; B. J. MacGowan; P. Michel; N. B. Meezan; L. J. Suter; S. Dixit; J. L. Kline; G. A. Kyrala; D. K. Bradley; D. A. Callahan; E. L. Dewald; L. Divol; E. G. Dzenitis; M. J. Edwards; Alex V. Hamza; C. A. Haynam; D. E. Hinkel; D. H. Kalantar; J. D. Kilkenny; O. L. Landen; J. D. Lindl; S. LePape; J. D. Moody; A. Nikroo; T. Parham; M. B. Schneider; R. P. J. Town; Paul J. Wegner; K. Widmann; Pamela K. Whitman

Ignition Set to Go One aim of the National Ignition Facility is to implode a capsule containing a deuterium-tritium fuel mix and initiate a fusion reaction. With 192 intense laser beams focused into a centimeter-scale cavity, a major challenge has been to create a symmetric implosion and the necessary temperatures within the cavity for ignition to be realized (see the Perspective by Norreys). Glenzer et al. (p. 1228, published online 28 January) now show that these conditions can be met, paving the way for the next step of igniting a fuel-filled capsule. Furthermore, Li et al. (p. 1231, published online 28 January) show how charged particles can be used to characterize and measure the conditions within the imploding capsule. The high energies and temperature realized can also be used to model astrophysical and other extreme energy processes in a laboratory settings. Laser-driven temperatures and implosion symmetry are close to the requirements for inertial-fusion ignition. Indirect-drive hohlraum experiments at the National Ignition Facility have demonstrated symmetric capsule implosions at unprecedented laser drive energies of 0.7 megajoule. One hundred and ninety-two simultaneously fired laser beams heat ignition-emulate hohlraums to radiation temperatures of 3.3 million kelvin, compressing 1.8-millimeter-diameter capsules by the soft x-rays produced by the hohlraum. Self-generated plasma optics gratings on either end of the hohlraum tune the laser power distribution in the hohlraum, which produces a symmetric x-ray drive as inferred from the shape of the capsule self-emission. These experiments indicate that the conditions are suitable for compressing deuterium-tritium–filled capsules, with the goal of achieving burning fusion plasmas and energy gain in the laboratory.


Physics of Plasmas | 2006

High-energy Kα radiography using high-intensity, short-pulse lasersa)

H.-S. Park; D. M. Chambers; H.-K. Chung; R. J. Clarke; R. Eagleton; E. Giraldez; T. Goldsack; R. Heathcote; N. Izumi; M.H. Key; J. A. King; J. A. Koch; O. L. Landen; A. Nikroo; P. K. Patel; D. Price; B. A. Remington; H. F. Robey; Richard Adolph Snavely; D Steinman; R.B. Stephens; C. Stoeckl; M. Storm; Max Tabak; W. Theobald; R. P. J. Town; J. E. Wickersham; B. Zhang

The characteristics of 22–40keV Kα x-ray sources are measured. These high-energy sources are produced by 100TW and petawatt high-intensity lasers and will be used to develop and implement workable radiography solutions to probe high-Z and dense materials for the high-energy density experiments. The measurements show that the Kα source size from a simple foil target is larger than 60μm, too large for most radiography applications. The total Kα yield is independent of target thicknesses, verifying that refluxing plays a major role in photon generation. Smaller radiating volumes emit brighter Kα radiation. One-dimensional radiography experiments using small-edge-on foils resolved 10μm features with high contrast. Experiments were performed to test a variety of small volume two-dimensional point sources such as cones, wires, and embedded wires, measured photon yields, and compared the measurements with predictions from hybrid-particle-in-cell simulations. In addition to high-energy, high-resolution backlighte...


Review of Scientific Instruments | 2004

Dante soft x-ray power diagnostic for National Ignition Facility

E. L. Dewald; K. M. Campbell; R. E. Turner; J. P. Holder; O. L. Landen; S. H. Glenzer; R. L. Kauffman; L. J. Suter; M. Landon; M. Rhodes; D. Lee

Soft x-ray power diagnostics are essential for measuring the total x-ray flux, radiation temperature, conversion efficiency, and albedo that define the energetics in indirect and direct drive, as well as other types of high temperature laser plasma experiments. A key diagnostic for absolute radiation flux and radiation temperature in hohlraum experiments is the Dante broadband soft x-ray spectrometer. For the extended range of x-ray fluxes predicted for National Ignition Facility (NIF) compared to Omega or Nova hohlraums, the Dante spectrometer for NIF will include more high energy (<2 keV) edge filter band-pass channels and access to an increased dynamic range using grids and signal division. This will allow measurements of radiation fluxes of between 0.01 to 100 TW/sr, for hohlraum radiation temperatures between 50 eV and 1 keV. The NIF Dante will include a central four-channel imaging line-of-sight to verify the source size, alignment as well as checking for any radiation contributions from unconverted...


Physics of Plasmas | 2011

The experimental plan for cryogenic layered target implosions on the National Ignition Facility—The inertial confinement approach to fusion

M. J. Edwards; J. D. Lindl; B. K. Spears; S. V. Weber; L. J. Atherton; D. L. Bleuel; David K. Bradley; D. A. Callahan; Charles Cerjan; D. S. Clark; G. W. Collins; J. Fair; R. J. Fortner; S. H. Glenzer; S. W. Haan; B. A. Hammel; Alex V. Hamza; S. P. Hatchett; N. Izumi; B. Jacoby; O. S. Jones; J. A. Koch; B. J. Kozioziemski; O. L. Landen; R. A. Lerche; B. J. MacGowan; A. J. Mackinnon; E. R. Mapoles; M. M. Marinak; M. J. Moran

Ignition requires precisely controlled, high convergence implosions to assemble a dense shell of deuterium-tritium (DT) fuel with ρR>∼1 g/cm2 surrounding a 10 keV hot spot with ρR ∼ 0.3 g/cm2. A working definition of ignition has been a yield of ∼1 MJ. At this yield the α-particle energy deposited in the fuel would have been ∼200 kJ, which is already ∼10 × more than the kinetic energy of a typical implosion. The National Ignition Campaign includes low yield implosions with dudded fuel layers to study and optimize the hydrodynamic assembly of the fuel in a diagnostics rich environment. The fuel is a mixture of tritium-hydrogen-deuterium (THD) with a density equivalent to DT. The fraction of D can be adjusted to control the neutron yield. Yields of ∼1014−15 14 MeV (primary) neutrons are adequate to diagnose the hot spot as well as the dense fuel properties via down scattering of the primary neutrons. X-ray imaging diagnostics can function in this low yield environment providing additional information about ...


Physics of Plasmas | 1996

Three-dimensional simulations of Nova high growth factor capsule implosion experiments

M. M. Marinak; R. E. Tipton; O. L. Landen; T. J. Murphy; Peter A. Amendt; S. W. Haan; Stephen P. Hatchett; C. J. Keane; R. McEachern; R. J. Wallace

Capsule implosion experiments carried out on the Nova laser [E. M. Campbell et al., Rev. Sci. Instrum. 57, 2101 (1986)] are simulated with the three‐dimensional HYDRA radiation hydrodynamics code [NTIS Document No. DE‐96004569 (M. M. Marinak et al. in UCRL‐LR‐105821‐95‐3)]. Simulations of ordered, near single mode perturbations indicate that structures which evolve into round spikes can penetrate farthest into the hot spot. Bubble‐shaped perturbations can burn through the capsule shell fastest, in which case they cause even more damage. A simulation of a capsule with a multimode perturbation of moderate amplitude shows spike amplitudes evolving in good agreement with a saturation model during the deceleration phase. The presence of sizable low mode asymmetry, caused either by drive asymmetry or perturbations in the capsule shell, can dramatically affect the manner in which spikes approach the center of the hot spot. Three‐dimensional coupling between the low mode shell perturbations intrinsic to Nova caps...


Physics of Plasmas | 2011

Capsule implosion optimization during the indirect-drive National Ignition Campaign

O. L. Landen; John Edwards; S. W. Haan; H. F. Robey; J. L. Milovich; B. K. Spears; S. V. Weber; D. S. Clark; J. D. Lindl; B. J. MacGowan; E. I. Moses; J. Atherton; Peter A. Amendt; T. R. Boehly; David K. Bradley; David G. Braun; D. A. Callahan; Peter M. Celliers; G. W. Collins; E. L. Dewald; L. Divol; J. A. Frenje; S. H. Glenzer; Alex V. Hamza; B. A. Hammel; D. G. Hicks; Nelson M. Hoffman; N. Izumi; O. S. Jones; J. D. Kilkenny

Capsule performance optimization campaigns will be conducted at the National Ignition Facility [G. H. Miller, E. I. Moses, and C. R. Wuest, Nucl. Fusion 44, 228 (2004)] to substantially increase the probability of ignition. The campaigns will experimentally correct for residual uncertainties in the implosion and hohlraum physics used in our radiation-hydrodynamic computational models using a variety of ignition capsule surrogates before proceeding to cryogenic-layered implosions and ignition experiments. The quantitative goals and technique options and down selections for the tuning campaigns are first explained. The computationally derived sensitivities to key laser and target parameters are compared to simple analytic models to gain further insight into the physics of the tuning techniques. The results of the validation of the tuning techniques at the OMEGA facility [J. M. Soures et al., Phys. Plasmas 3, 2108 (1996)] under scaled hohlraum and capsule conditions relevant to the ignition design are shown ...


Science | 2008

Ultrafast x-ray Thomson scattering of shock-compressed matter.

A. L. Kritcher; Paul Neumayer; John I. Castor; T. Döppner; R. W. Falcone; O. L. Landen; Haeja Lee; R.W. Lee; Edward C. Morse; A. Ng; Steve Pollaine; D. Price; S. H. Glenzer

Spectrally resolved scattering of ultrafast K-α x-rays has provided experimental validation of the modeling of the compression and heating of shocked matter. The elastic scattering component has characterized the evolution and coalescence of two shocks launched by a nanosecond laser pulse into lithium hydride with an unprecedented temporal resolution of 10 picoseconds. At shock coalescence, we observed rapid heating to temperatures of 25,000 kelvin when the scattering spectra show the collective plasmon oscillations that indicate the transition to the dense metallic plasma state. The plasmon frequency determines the material compression, which is found to be a factor of 3, thereby reaching conditions in the laboratory relevant for studying the physics of planetary formation.

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S. H. Glenzer

SLAC National Accelerator Laboratory

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E. L. Dewald

Lawrence Livermore National Laboratory

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D. A. Callahan

Lawrence Livermore National Laboratory

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S. W. Haan

Lawrence Livermore National Laboratory

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N. B. Meezan

Lawrence Livermore National Laboratory

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B. A. Hammel

Lawrence Livermore National Laboratory

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L. J. Suter

Lawrence Livermore National Laboratory

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N. Izumi

Lawrence Livermore National Laboratory

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O. S. Jones

Lawrence Livermore National Laboratory

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