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Dive into the research topics where E. Dewald is active.

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Featured researches published by E. Dewald.


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.


Physics of Plasmas | 2010

Multi-keV x-ray source development experiments on the National Ignition Facility

K. B. Fournier; M. J. May; Jeffrey D. Colvin; Jave O. Kane; M. B. Schneider; E. Dewald; C. A. Thomas; S. Compton; R. Marrs; J. D. Moody; E. Bond; P. Michel; J. H. Fisher; C. D. Newlander; J. F. Davis

We report results from a five shot campaign carried out with Ar–Xe gas-filled targets at the National Ignition Facility (NIF). The targets were shot with ≈350 kJ of 3ω laser energy delivered with a 5 ns trapezoidal laser pulse. We report measured x-ray output from the target in different spectral bands both below and above 1.5 keV photon energies: We find yields of ≈20.5 kJ/sr with peak x-ray power approaching 4 TW/sr over all energies, as measured for the unique viewing angle of our detector, and ≈3.6 kJ/sr with peak x-ray power of 1 TW/sr for x-rays with energies >3 keV. This is a laser-to-x-ray conversion efficiency of 13±1.3% for isotropic x-rays with energies >3 keV. Laser energy reflected by the target plasma for both inner and outer-cone beams is measured and found to be small, between 1% and 4% of the drive energy. The energy emitted in hard x-rays (with energies >25 keV) is measured and found to be ≈1 J/sr. Two-dimensional imaging of the target plasma during the laser pulse confirms a fast, volum...


Physics of Plasmas | 2007

Amplification of an ultrashort pulse laser by stimulated Raman scattering of a 1ns pulse in a low density plasma

R. K. Kirkwood; E. Dewald; C. Niemann; N. B. Meezan; S. C. Wilks; D. W. Price; O. L. Landen; Jonathan S. Wurtele; Andrew Emile Charman; R. R. Lindberg; N. J. Fisch; V. M. Malkin; E. O. Valeo

Experiments are described in which a 1mJ, 1ps, 1200nm seed laser beam is amplified by the interaction with an intersecting 350J, 1ns, 1054nm pump beam in a low density (1×1019∕cm3) plasma. The transmission of the seed beam is observed to be enhanced by ≳25× when the plasma is near the resonant density for stimulated Raman scattering, compared to measured transmissions at wavelengths just below the resonant value. The amplification is observed to increase rapidly with increases in both pump intensity and plasma density.


Review of Scientific Instruments | 2012

Charged-particle spectroscopy for diagnosing shock ρR and strength in NIF implosions

A. B. Zylstra; J. A. Frenje; F. H. Séguin; M. Rosenberg; H. G. Rinderknecht; M. Gatu Johnson; D. T. Casey; N. Sinenian; M. J.-E. Manuel; C. Waugh; H. Sio; C. K. Li; R. D. Petrasso; S. Friedrich; K. M. Knittel; R. Bionta; M. McKernan; D. A. Callahan; G. W. Collins; E. Dewald; T. Döppner; M. J. Edwards; S. H. Glenzer; Damien G. Hicks; O. L. Landen; Richard A. London; A. J. Mackinnon; N. B. Meezan; Rajendra Prasad; J. E. Ralph

The compact Wedge Range Filter (WRF) proton spectrometer was developed for OMEGA and transferred to the National Ignition Facility (NIF) as a National Ignition Campaign diagnostic. The WRF measures the spectrum of protons from D-(3)He reactions in tuning-campaign implosions containing D and (3)He gas; in this work we report on the first proton spectroscopy measurement on the NIF using WRFs. The energy downshift of the 14.7-MeV proton is directly related to the total ρR through the plasma stopping power. Additionally, the shock proton yield is measured, which is a metric of the final merged shock strength.


Physics of Plasmas | 2016

The near vacuum hohlraum campaign at the NIF: A new approach

S. Le Pape; L. Berzak Hopkins; L. Divol; N. B. Meezan; D. Turnbull; A. J. Mackinnon; D. Ho; J. S. Ross; S. F. Khan; A. Pak; E. Dewald; L.R. Benedetti; S. R. Nagel; J. Biener; D. A. Callahan; C. B. Yeamans; P. Michel; M. B. Schneider; B. J. Kozioziemski; T. Ma; A. G. MacPhee; S. W. Haan; N. Izumi; R. Hatarik; P. A. Sterne; Peter M. Celliers; J. E. Ralph; Ryan Rygg; D. J. Strozzi; J. D. Kilkenny

The near vacuum campaign on the National Ignition Facility has concentrated its efforts over the last year on finding the optimum target geometry to drive a symmetric implosion at high convergence ratio (30×). As the hohlraum walls are not tamped with gas, the hohlraum is filling with gold plasma and the challenge resides in depositing enough energy in the hohlraum before it fills up. Hohlraum filling is believed to cause symmetry swings late in the pulse that are detrimental to the symmetry of the hot spot at high convergence. This paper describes a series of experiments carried out to examine the effect of increasing the distance between the hohlraum wall and the capsule (case to capsule ratio) on the symmetry of the hot spot. These experiments have shown that smaller Case to Capsule Ratio (CCR of 2.87 and 3.1) resulted in oblate implosions that could not be tuned round. Larger CCR (3.4) led to a prolate implosion at convergence 30× implying that inner beam propagation at large CCR is not impeded by the expanding hohlraum plasma. A Case to Capsule ratio of 3.4 is a promising geometry to design a round implosion but in a smaller hohlraum where the hohlraum losses are lower, enabling a wider cone fraction range to adjust symmetry.


Physics of Plasmas | 2011

Multi-beam effects on backscatter and its saturation in experiments with conditions relevant to ignitiona)

R. K. Kirkwood; P. Michel; Richard A. London; J. D. Moody; E. Dewald; L. Yin; J. L. Kline; D. E. Hinkel; D. A. Callahan; N. B. Meezan; E. A. Williams; L. Divol; B. L. Albright; K. J. Bowers; E. Bond; Harvey A. Rose; Y. Ping; T. L. Wang; C. Joshi; W. Seka; N. J. Fisch; D. Turnbull; S. Suckewer; Jonathan S. Wurtele; S. H. Glenzer; L. J. Suter; C. A. Haynam; O. L. Landen; B. J. MacGowan

To optimize the coupling to indirect drive targets in the National Ignition Campaign (NIC) at the National Ignition Facility [E. Moses et al., Phys. Plasmas 16, 041006 (2009)], a model of stimulated scattering produced by multiple laser beams is used. The model has shown that scatter of the 351 nm beams can be significantly enhanced over single beam predictions in ignition relevant targets by the interaction of the multiple crossing beams with a millimeter scale length, 2.5 keV, 0.02−0.05 × critical density, plasma. The model uses a suite of simulation capabilities and its key aspects are benchmarked with experiments at smaller laser facilities. The model has also influenced the design of the initial targets used for NIC by showing that both the stimulated Brillouin scattering (SBS) and stimulated Raman scattering (SRS) can be reduced by the reduction of the plasma density in the beam intersection volume that is caused by an increase in the diameter of the laser entrance hole (LEH). In this model, a linea...


Physics of Plasmas | 2013

Radiative shocks produced from spherical cryogenic implosions at the National Ignition Facility

A. Pak; L. Divol; G. Gregori; S. V. Weber; J. Atherton; R. Bennedetti; D. K. Bradley; D. A. Callahan; D. T. Casey; E. Dewald; T. Döppner; M. J. Edwards; J. A. Frenje; S. Glenn; G. P. Grim; Damien G. Hicks; W. W. Hsing; N. Izumi; O. S. Jones; Maria Gatu Johnson; S. F. Khan; J. D. Kilkenny; J. L. Kline; G. A. Kyrala; J. D. Lindl; O. L. Landen; S. Le Pape; T. Ma; A. G. MacPhee; B. J. MacGowan

Spherically expanding radiative shock waves have been observed from inertially confined implosion experiments at the National Ignition Facility. In these experiments, a spherical fusion target, initially 2 mm in diameter, is compressed via the pressure induced from the ablation of the outer target surface. At the peak compression of the capsule, x-ray and nuclear diagnostics indicate the formation of a central core, with a radius and ion temperature of ∼20 μm and ∼ 2 keV, respectively. This central core is surrounded by a cooler compressed shell of deuterium-tritium fuel that has an outer radius of ∼40 μm and a density of >500 g/cm3. Using inputs from multiple diagnostics, the peak pressure of the compressed core has been inferred to be of order 100 Gbar for the implosions discussed here. The shock front, initially located at the interface between the high pressure compressed fuel shell and surrounding in-falling low pressure ablator plasma, begins to propagate outwards after peak compression has been rea...


Physics of Plasmas | 2009

Sensitivity of ignition scale backlit thin-shell implosions to hohlraum symmetry in the foot of the drive pulse

R. K. Kirkwood; J. L. Milovich; David K. Bradley; Mark J. Schmitt; S. R. Goldman; D. H. Kalantar; D. Meeker; O. S. Jones; Stephen M. Pollaine; Peter A. Amendt; E. Dewald; John Edwards; O. Landen; A. Nikroo

A necessary condition for igniting indirectly driven inertial confinement fusion spherical capsules on the National Ignition Facility (NIF) is controlling drive flux asymmetry to the 1% level time-integrated over the pulse and with <10%∕ns swings during the pulse [J. D. Lindl, P. Amendt, R. L. Berger et al., Phys. Plasmas 11, 339 (2003)]. While drive symmetry during the first 2ns of the pulse can be inferred by using the re-emission pattern from a surrogate high Z sphere and symmetry during the last 5ns inferred from the shape of fully imploded capsules, the midportion (≈2–10ns) has been shown to be amenable to detection by the in-flight shape of x-ray backlit thin-shell capsules. In this paper, we present sensitivity studies conducted on the University of Rochester’s OMEGA laser [J. Soures, R. L. McCrory, C. P. Verdon et al., Phys. Plasmas 3, 2108 (1996)] of the thin-shell symmetry measurement technique at near NIF-scale for two candidate capsule ablator materials: Ge-doped CH and Cu-doped Be. These expe...


Review of Scientific Instruments | 2010

Characterizing high energy spectra of NIF ignition Hohlraums using a differentially filtered high energy multipinhole x-ray imager.

Hye-Sook Park; E. Dewald; S. H. Glenzer; D. H. Kalantar; J. D. Kilkenny; B. J. MacGowan; Brian Maddox; J. L. Milovich; R. Prasad; B. A. Remington; H. F. Robey; C. A. Thomas

Understanding hot electron distributions generated inside Hohlraums is important to the national ignition campaign for controlling implosion symmetry and sources of preheat. While direct imaging of hot electrons is difficult, their spatial distribution and spectrum can be deduced by detecting high energy x-rays generated as they interact with target materials. We used an array of 18 pinholes with four independent filter combinations to image entire Hohlraums with a magnification of 0.87× during the Hohlraum energetics campaign on NIF. Comparing our results with Hohlraum simulations indicates that the characteristic 10-40 keV hot electrons are mainly generated from backscattered laser-plasma interactions rather than from Hohlraum hydrodynamics.


Physics of Plasmas | 2018

Implosion shape control of high-velocity, large case-to-capsule ratio beryllium ablators at the National Ignition Facility

E. N. Loomis; S. A. Yi; G. A. Kyrala; J. L. Kline; Andrei N. Simakov; J. E. Ralph; M. Millot; E. Dewald; A. Zylstra; J. R. Rygg; Peter M. Celliers; C. Goyon; B. Lahmann; H. Sio; S. A. MacLaren; L. Masse; D. A. Callahan; O. A. Hurricane; D. C. Wilson; N. Rice; H. Huang; C. Kong; J. Bae; A. Nikroo; S. H. Batha

Experiments at the National Ignition Facility (NIF) show that the implosion shape of inertial confinement fusion ablators is a key factor limiting performance. To achieve more predictable, shape tunable implosions, we have designed and fielded a large 4.2 case-to-capsule ratio target at the NIF using 6.72 mm diameter Au hohlraums and 1.6 mm diameter Cu-doped Be capsules. Simulations show that at these dimensions during a 10 ns 3-shock laser pulse reaching 275 eV hohlraum temperatures, the plasma flow from the hohlraum wall and ablator is not significant enough to impede beam propagation. Experiments measuring the shock symmetry and in-flight shell symmetry closely matched the simulations. Most notably, in two experiments, we demonstrated symmetry control from negative to positive Legendre P2 space by varying the inner to total laser power cone fraction by 5% below and above the predicted symmetric value. Some discrepancies found in 1st shock arrival times that could affect agreement in late time implosion symmetry suggest hohlraum and capsule modeling uncertainties do remain, but this target design reduces sensitivities to them.Experiments at the National Ignition Facility (NIF) show that the implosion shape of inertial confinement fusion ablators is a key factor limiting performance. To achieve more predictable, shape tunable implosions, we have designed and fielded a large 4.2 case-to-capsule ratio target at the NIF using 6.72 mm diameter Au hohlraums and 1.6 mm diameter Cu-doped Be capsules. Simulations show that at these dimensions during a 10 ns 3-shock laser pulse reaching 275 eV hohlraum temperatures, the plasma flow from the hohlraum wall and ablator is not significant enough to impede beam propagation. Experiments measuring the shock symmetry and in-flight shell symmetry closely matched the simulations. Most notably, in two experiments, we demonstrated symmetry control from negative to positive Legendre P2 space by varying the inner to total laser power cone fraction by 5% below and above the predicted symmetric value. Some discrepancies found in 1st shock arrival times that could affect agreement in late time implosion...

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O. L. Landen

Lawrence Livermore National Laboratory

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J. L. Milovich

Lawrence Livermore National Laboratory

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J. E. Ralph

Lawrence Livermore National Laboratory

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N. B. Meezan

Lawrence Livermore National Laboratory

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D. A. Callahan

Lawrence Livermore National Laboratory

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L. Divol

Lawrence Livermore National Laboratory

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C. A. Thomas

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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T. Ma

Lawrence Livermore National Laboratory

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