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Featured researches published by K. Widmann.


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.


The Astrophysical Journal | 1998

Laboratory Measurements and Modeling of the Fe XVII X-Ray Spectrum

Gregory Vallee Brown; P. Beiersdorfer; Duane A. Liedahl; K. Widmann; Steven M. Kahn

Detailed measurements, line identifications, and modeling calculations of the Fe XVII L-shell emission spectrum between 9.8 and 17.5 A are presented. The measurements were carried out on an electron beam ion trap under precisely controlled conditions where electron-impact excitation followed by radiative cascades is the dominant line formation process. In addition to the strong transitions emanating from the n = 3 shell, we identify and accurately determine wavelengths for transitions from higher shells up to n = 11, including two electric quadrupole transitions that have not been previously identified. Various theoretical values, including new distorted wave calculations, are compared to our measurements, which establish definitive values for testing spectral modeling predictions. We find a value of 3.04 ± 0.12 for the ratio of the intensity of the 2p-3d1P1 resonance and of the 2p-3d3D1 intercombination line situated at 15.01 and 15.26 A, respectively. This value is higher than the values observed in solar spectra, which supports claims that the solar value is affected by resonant scattering. However, because our value is significantly lower than calculated values, the amount of scattering has probably been overestimated in past analyses. Comparisons of the measured intensity ratios of the transitions originating in levels of higher principal quantum number n with present distorted wave calculations show good agreement up to n = 6. The combined flux of all 2p-nd transitions with n ≥ 5 and all 2s-np transitions with n = 4 and 5 relative to the flux of the 15.01 A resonance line has been measured to be 0.13+ 0.04−0.03 .


Physics of Plasmas | 2010

Symmetry tuning via controlled crossed-beam energy transfer on the National Ignition Facilitya)

P. Michel; S. H. Glenzer; L. Divol; David K. Bradley; D. A. Callahan; S. Dixit; S. Glenn; D. E. Hinkel; R. K. Kirkwood; J. L. Kline; W. L. Kruer; G. A. Kyrala; S. Le Pape; N. B. Meezan; R. P. J. Town; K. Widmann; E. A. Williams; B. J. MacGowan; J. D. Lindl; L. Suter

The Hohlraum energetics experimental campaign started in the summer of 2009 on the National Ignition Facility (NIF) [E. I. Moses et al., Phys. Plasmas 16, 041006 (2009)]. These experiments showed good coupling of the laser energy into the targets [N. Meezan et al., Phys. Plasmas 17, 056304 (2010)]. They have also demonstrated controlled crossed-beam energy transfer between laser beams as an efficient and robust tool to tune the implosion symmetry of ignition capsules, as predicted by earlier calculations [P. Michel et al., Phys. Rev. Lett. 102, 025004 (2009)]. A new linear model calculating crossed-beam energy transfer between cones of beams on the NIF has been developed. The model has been applied to the subscale Hohlraum targets shot during the National Ignition Campaign in 2009. A good agreement can be found between the calculations and the experiments when the impaired propagation of the laser beams due to backscatter is accounted for.


Physics of Plasmas | 2014

The high-foot implosion campaign on the National Ignition Facilitya)

O. A. Hurricane; D. A. Callahan; D. T. Casey; E. L. Dewald; T. R. Dittrich; T. Döppner; M. A. Barrios Garcia; D. E. Hinkel; L. Berzak Hopkins; P. Kervin; J. L. Kline; S. Le Pape; T. Ma; A. G. MacPhee; J. L. Milovich; J. D. Moody; A. Pak; P. K. Patel; H.-S. Park; B. A. Remington; H. F. Robey; J. D. Salmonson; P. T. Springer; R. Tommasini; L. R. Benedetti; J. A. Caggiano; Peter M. Celliers; C. Cerjan; Rebecca Dylla-Spears; D. H. Edgell

The “High-Foot” platform manipulates the laser pulse-shape coming from the National Ignition Facility laser to create an indirect drive 3-shock implosion that is significantly more robust against instability growth involving the ablator and also modestly reduces implosion convergence ratio. This strategy gives up on theoretical high-gain in an inertial confinement fusion implosion in order to obtain better control of the implosion and bring experimental performance in-line with calculated performance, yet keeps the absolute capsule performance relatively high. In this paper, we will cover the various experimental and theoretical motivations for the high-foot drive as well as cover the experimental results that have come out of the high-foot experimental campaign. At the time of this writing, the high-foot implosion has demonstrated record total deuterium-tritium yields (9.3×1015) with low levels of inferred mix, excellent agreement with implosion simulations, fuel energy gains exceeding unity, and evidenc...


Physics of Plasmas | 2010

National Ignition Campaign Hohlraum energetics

N. B. Meezan; L. J. Atherton; D. A. Callahan; E. L. Dewald; S. Dixit; E. G. Dzenitis; M. J. Edwards; C. A. Haynam; D. E. Hinkel; O. S. Jones; O. L. Landen; Richard A. London; P. Michel; J. D. Moody; J. L. Milovich; M. B. Schneider; C. A. Thomas; R. P. J. Town; A. Warrick; S. V. Weber; K. Widmann; S. H. Glenzer; L. J. Suter; B. J. MacGowan; J. L. Kline; George A. Kyrala; A. Nikroo

The first series of experiments of the National Ignition Facility (NIF) [E. I. Moses et al., Phys. Plasmas 16, 041006 (2009)] tested ignition Hohlraum “energetics,” a term described by four broad goals: (1) measurement of laser absorption by the Hohlraum; (2) measurement of the x-ray radiation flux (TRAD4) on the surrogate ignition capsule; (3) quantitative understanding of the laser absorption and resultant x-ray flux; and (4) determining whether initial Hohlraum performance is consistent with requirements for ignition. This paper summarizes the status of NIF Hohlraum energetics experiments. The Hohlraum targets and experimental design are described, as well as the results of the initial experiments. The data demonstrate low backscattered energy (<10%) for Hohlraums filled with helium gas. A discussion of our current understanding of NIF Hohlraum x-ray drive follows, including an overview of the computational tools, i.e., radiation-hydrodynamics codes that have been used to design the Hohlraums. The perf...


Physics of Plasmas | 2012

Implosion dynamics measurements at the National Ignition Facility

Damien G. Hicks; N. B. Meezan; E. L. Dewald; A. J. Mackinnon; R.E. Olson; D. A. Callahan; T. Döppner; L. R. Benedetti; D. K. Bradley; Peter M. Celliers; D. S. Clark; P. Di Nicola; S. N. Dixit; E. G. Dzenitis; J. E. Eggert; D. R. Farley; J. A. Frenje; S. Glenn; S. H. Glenzer; Alex V. Hamza; R. F. Heeter; J. P. Holder; N. Izumi; D. H. Kalantar; S. F. Khan; J. L. Kline; J. J. Kroll; G. A. Kyrala; T. Ma; A. G. MacPhee

Measurements have been made of the in-flight dynamics of imploding capsules indirectly driven by laser energies of 1–1.7 MJ at the National Ignition Facility [Miller et al., Nucl. Fusion 44, 228 (2004)]. These experiments were part of the National Ignition Campaign [Landen et al., Phys. Plasmas 18, 051002 (2011)] to iteratively optimize the inputs required to achieve thermonuclear ignition in the laboratory. Using gated or streaked hard x-ray radiography, a suite of ablator performance parameters, including the time-resolved radius, velocity, mass, and thickness, have been determined throughout the acceleration history of surrogate gas-filled implosions. These measurements have been used to establish a dynamically consistent model of the ablative drive history and shell compressibility throughout the implosion trajectory. First results showed that the peak velocity of the original 1.3-MJ Ge-doped polymer (CH) point design using Au hohlraums reached only 75% of the required ignition velocity. Several capsu...


Physics of Plasmas | 2012

A high-resolution integrated model of the National Ignition Campaign cryogenic layered experiments

O. S. Jones; C. Cerjan; M. M. Marinak; J. L. Milovich; H. F. Robey; P. T. Springer; L. R. Benedetti; D. L. Bleuel; E. Bond; D. K. Bradley; D. A. Callahan; J. A. Caggiano; Peter M. Celliers; D. S. Clark; S. M. Dixit; T. Döppner; Rebecca Dylla-Spears; E. G. Dzentitis; D. R. Farley; S. Glenn; S. H. Glenzer; S. W. Haan; B. J. Haid; C. A. Haynam; Damien G. Hicks; B. J. Kozioziemski; K. N. LaFortune; O. L. Landen; E. R. Mapoles; A. J. Mackinnon

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 measu...


Physics of Plasmas | 2012

Shock timing experiments on the National Ignition Facility: Initial results and comparison with simulation

H. F. Robey; T. R. Boehly; Peter M. Celliers; Jon H. Eggert; Damien G. Hicks; R.F. Smith; R. Collins; M. W. Bowers; K. Krauter; P. S. Datte; D. H. Munro; J. L. Milovich; O. S. Jones; P. Michel; C. A. Thomas; R.E. Olson; Stephen M. Pollaine; R. P. J. Town; S. W. Haan; D. A. Callahan; D. S. Clark; J. Edwards; J. L. Kline; S. N. Dixit; M. B. Schneider; E. L. Dewald; K. Widmann; J. D. Moody; T. Döppner; H.B. Radousky

Capsule implosions on the National Ignition Facility (NIF) [Lindl et al., Phys. Plasmas 11, 339 (2004)] are underway with the goal of compressing deuterium-tritium (DT) fuel to a sufficiently high areal density (ρR) to sustain a self-propagating burn wave required for fusion power gain greater than unity. These implosions are driven with a carefully tailored sequence of four shock waves that must be timed to very high precision in order to keep the DT fuel on a low adiabat. Initial experiments to measure the strength and relative timing of these shocks have been conducted on NIF in a specially designed surrogate target platform known as the keyhole target. This target geometry and the associated diagnostics are described in detail. The initial data are presented and compared with numerical simulations. As the primary goal of these experiments is to assess and minimize the adiabat in related DT implosions, a methodology is described for quantifying the adiabat from the shock velocity measurements. Results ...


Review of Scientific Instruments | 1996

The magnetic trapping mode of an electron beam ion trap: New opportunities for highly charged ion research

P. Beiersdorfer; L. Schweikhard; J. R. Crespo López-Urrutia; K. Widmann

Using x‐ray spectroscopic techniques, we have investigated the properties of an electron beam ion trap (EBIT) after the electron beam is switched off. In the absence of the electron beam, bare, and hydrogenlike Kr35+ and Kr36+ ions remain trapped due to externally applied magnetic and electric fields for at least 5 s; xenon ions with an open L shell, i.e., Xe45+–Xe52+, remain trapped at least as long as 20 s. The ion storage time in this ‘‘magnetic trapping mode’’ depends on the pressure of background atoms as well as on the value of the externally applied trapping potential, and even longer ion storage times appear possible. The magnetic trapping mode enables a variety of new opportunities for atomic physics research involving highly charged ions, which include the study of charge transfer reactions, Doppler‐shift‐free measurements of the Lamb shift, measurements of radiative lifetimes of long‐lived metastable levels, or ion‐ion collision studies, by x‐ray or laser spectroscopy, and mass spectrometry. Be...


Review of Scientific Instruments | 2006

Soft x-ray power diagnostic improvements at the Omega Laser Facility

C. Sorce; Jochen Schein; F. Weber; K. Widmann; K. M. Campbell; E. Dewald; R. E. Turner; O. L. Landen; K. Jacoby; P. Torres; D. Pellinen

Soft x-ray power diagnostics are essential for evaluating high temperature laser plasma experiments. The Dante soft x-ray spectrometer, a core diagnostic for radiation flux and temperature measurements of Hohlraums, installed on the Omega Laser Facility at the Laboratory for Laser Energetics has recently undergone a series of upgrades. Work performed at Brookhaven National Laboratory for the development of the National Ignition Facility (NIF) Dante spectrometer enables the Omega Dante to offer a total of 18 absolutely calibrated channels in the energy range from 50eVto20keV. This feature provides Dante with the capability to measure higher, NIF relevant, radiation temperatures with increased accuracy including a differentiation of higher energy radiation such as the Au M and L bands. Diagnostic monitoring using experimental data from directly driven Au spherical shots is discussed.

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P. Beiersdorfer

Lawrence Livermore National Laboratory

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M. B. Schneider

Lawrence Livermore National Laboratory

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D. A. Callahan

Lawrence Livermore National Laboratory

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O. L. Landen

Lawrence Livermore National Laboratory

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N. B. Meezan

Lawrence Livermore National Laboratory

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D. E. Hinkel

Lawrence Livermore National Laboratory

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J. D. Moody

Lawrence Livermore National Laboratory

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E. L. Dewald

Lawrence Livermore National Laboratory

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J. L. Kline

Los Alamos National Laboratory

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P. Michel

Lawrence Livermore National Laboratory

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