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Featured researches published by L. R. Benedetti.


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 | 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 | 2014

Dynamic symmetry of indirectly driven inertial confinement fusion capsules on the National Ignition Facilitya)

R. P. J. Town; D. K. Bradley; A. L. Kritcher; O. S. Jones; J. R. Rygg; R. Tommasini; M. A. Barrios; L. R. Benedetti; L. Berzak Hopkins; Peter M. Celliers; T. Döppner; E. L. Dewald; David C. Eder; J. E. Field; S. M. Glenn; N. Izumi; S. W. Haan; S. F. Khan; J. L. Kline; G. A. Kyrala; T. Ma; J. L. Milovich; J. D. Moody; S. R. Nagel; A. Pak; J. L. Peterson; H. F. Robey; J. S. Ross; R. H. H. Scott; B. K. Spears

In order to achieve ignition using inertial confinement fusion it is important to control the growth of low-mode asymmetries as the capsule is compressed. Understanding the time-dependent evolution of the shape of the hot spot and surrounding fuel layer is crucial to optimizing implosion performance. A design and experimental campaign to examine sources of asymmetry and to quantify symmetry throughout the implosion has been developed and executed on the National Ignition Facility (NIF) [E. I. Moses et al., Phys. Plasmas 16, 041006 (2009)]. We have constructed a large simulation database of asymmetries applied during different time intervals. Analysis of the database has shown the need to measure and control the hot-spot shape, areal density distribution, and symmetry swings during the implosion. The shape of the hot spot during final stagnation is measured using time-resolved imaging of the self-emission, and information on the shape of the fuel at stagnation can be obtained from Compton radiography [R. Tommasini et al., Phys. Plasmas 18, 056309 (2011)]. For the first time on NIF, two-dimensional inflight radiographs of gas-filled and cryogenic fuel layered capsules have been measured to infer the symmetry of the radiation drive on the capsule. These results have been used to modify the hohlraum geometry and the wavelength tuning to improve the inflight implosion symmetry. We have also expanded our shock timing capabilities by the addition of extra mirrors inside the re-entrant cone to allow the simultaneous measurement of shock symmetry in three locations on a single shot, providing asymmetry information up to Legendre mode 4. By diagnosing the shape at nearly every step of the implosion, we estimate that shape has typically reduced fusion yield by about 50% in ignition experiments.


Physics of Plasmas | 2012

The velocity campaign for ignition on NIF

D. A. Callahan; N. B. Meezan; S. H. Glenzer; A. J. Mackinnon; L. R. Benedetti; D. K. Bradley; J. Celeste; Peter M. Celliers; S. N. Dixit; T. Döppner; E. G. Dzentitis; S. Glenn; S. W. Haan; C. A. Haynam; Damien G. Hicks; D. E. Hinkel; O. S. Jones; O. L. Landen; Richard A. London; A. G. MacPhee; P. Michel; J. D. Moody; J. E. Ralph; H. F. Robey; M. D. Rosen; M. B. Schneider; D. J. Strozzi; L. J. Suter; R. P. J. Town; K. Widmann

Achieving inertial confinement fusion ignition requires a symmetric, high velocity implosion. Experiments show that we can reach 95 ± 5% of the required velocity by using a 420 TW, 1.6 MJ laser pulse. In addition, experiments with a depleted uranium hohlraum show an increase in capsule performance which suggests an additional 18 ± 5 μm/ns of velocity with uranium hohlraums over gold hohlraums. Combining these two would give 99 ± 5% of the ignition velocity. Experiments show that we have the ability to tune symmetry using crossbeam transfer. We can control the second Legendre mode (P2) by changing the wavelength separation between the inner and outer cones of laser beams. We can control the azimuthal m = 4 asymmetry by changing the wavelength separation between the 23.5 and 30 degree beams on NIF. This paper describes our “first pass” tuning the implosion velocity and shape on the National Ignition Facility laser [Moses et al., Phys. Plasmas, 16, 041006 (2009)].


Physics of Plasmas | 2015

Effect of the mounting membrane on shape in inertial confinement fusion implosions

S. R. Nagel; S. W. Haan; J. R. Rygg; M. A. Barrios; L. R. Benedetti; D. K. Bradley; J. E. Field; B. A. Hammel; N. Izumi; O. S. Jones; S. F. Khan; T. Ma; A. Pak; R. Tommasini; R. P. J. Town

The performance of Inertial Confinement Fusion targets relies on the symmetric implosion of highly compressed fuel. X-ray area-backlit imaging is used to assess in-flight low mode 2D asymmetries of the shell. These time-resolved images of the shell exhibit features that can be related to the lift-off position of the membranes used to hold the capsule within the hohlraum. Here, we describe a systematic study of this membrane or “tent” thickness and its impact on the measured low modes for in-flight and self-emission images. The low mode amplitudes of the shell in-flight shape (P2 and P4) are weakly affected by the tent feature in time-resolved, backlit data. By contrast, time integrated self-emission images along the same axis exhibit a reversal in perceived P4 mode due to growth of a feature seeded by the tent, which can explain prior inconsistencies between the in-flight P4 and core P4, leading to a reevaluation of optimum hohlraum length. Simulations with a tent-like feature normalized to match the feat...


Physics of Plasmas | 2015

Tent-induced perturbations on areal density of implosions at the National Ignition Facilitya)

R. Tommasini; J. E. Field; B. A. Hammel; O. L. Landen; S. W. Haan; C. Aracne-Ruddle; L. R. Benedetti; D. K. Bradley; D. A. Callahan; E. L. Dewald; T. Doeppner; M. J. Edwards; O. A. Hurricane; N. Izumi; O. A. Jones; T. Ma; N. B. Meezan; S. R. Nagel; J. R. Rygg; K. Segraves; Michael Stadermann; R. J. Strauser; R. P. J. Town

Areal density non-uniformities seeded by time-dependent drive variations and target imperfections in Inertial Confinement Fusion (ICF) targets can grow in time as the capsule implodes, with growth rates that are amplified by instabilities. Here, we report on the first measurements of the perturbations on the density and areal density profiles induced by the membranes used to hold the capsule within the hohlraum in indirect drive ICF targets. The measurements are based on the reconstruction of the ablator density profiles from 2D radiographs obtained using pinhole imaging coupled to area backlighting, as close as 150 ps to peak compression. Our study shows a clear correlation between the modulations imposed on the areal density and measured neutron yield, and a 3× reduction in the areal density perturbations comparing a high-adiabat vs. low-adiabat pulse shape.


Physics of Plasmas | 2017

Symmetry control of an indirectly driven high-density-carbon implosion at high convergence and high velocity

L. Divol; A. Pak; L. Berzak Hopkins; S. Le Pape; N. B. Meezan; E. L. Dewald; D. Ho; S. F. Khan; A. J. Mackinnon; J. S. Ross; D. P. Turnbull; C. R. Weber; Peter M. Celliers; M. Millot; L. R. Benedetti; J. E. Field; N. Izumi; G. A. Kyrala; T. Ma; S. R. Nagel; J. R. Rygg; D. H. Edgell; A. G. MacPhee; C. Goyon; M. Hohenberger; B. J. MacGowan; P. Michel; D. J. Strozzi; W. S. Cassata; D. T. Casey

We report on the most recent and successful effort at controlling the trajectory and symmetry of a high density carbon implosion at the National Ignition Facility. We use a low gasfill (0.3 mg/cc He) bare depleted uranium hohlraum with around 1 MJ of laser energy to drive a 3-shock-ignition relevant implosion. We assess drive performance and we demonstrate symmetry control at convergence 1, 3–5, 12, and 27 to better than ±5 μm using a succession of experimental platforms. The symmetry control was maintained at a peak fuel velocity of 380 km/s. Overall, implosion symmetry measurements are consistent with the pole-equator symmetry of the X-ray drive on the capsule being better than 5% in the foot of the drive (when shocks are launched) and better than 1% during peak drive (main acceleration phase). This level of residual asymmetry should have little impact on implosion performance.


Review of Scientific Instruments | 2012

Extracting core shape from x-ray images at the National Ignition Facility.

S. Glenn; L. R. Benedetti; D. K. Bradley; B. A. Hammel; N. Izumi; S. F. Khan; G. A. Kyrala; T. Ma; J. L. Milovich; A. Pak; V. A. Smalyuk; R. Tommasini; R. P. J. Town

Measuring the shape of implosions is critical to inertial confinement fusion experiments at the National Ignition Facility. We have developed techniques that have proven successful for extracting shape information from images of x-ray self-emission recorded by a variety of diagnostic instruments for both DT-filled targets and low-yield surrogates. These key results help determine optimal laser and target parameters leading to ignition. We have compensated for instrumental response and have employed a variety of image processing methods to remove artifacts from the images while retaining salient features. The implosion shape has been characterized by decomposing intensity contours into Fourier and Legendre modes for different lines of sight. We also describe procedures we have developed for estimating uncertainties in these measurements.


Physics of Plasmas | 2015

Higher velocity, high-foot implosions on the National Ignition Facility lasera)

D. A. Callahan; O. A. Hurricane; D. E. Hinkel; T. Döppner; T. Ma; H.-S. Park; M. A. Barrios Garcia; L. Berzak Hopkins; D. T. Casey; C. Cerjan; E. L. Dewald; T. R. Dittrich; M. J. Edwards; S. W. Haan; Alex V. Hamza; J. L. Kline; J. P. Knauer; A. L. Kritcher; O. L. Landen; S. LePape; A. G. MacPhee; J. L. Milovich; A. Nikroo; A. Pak; P. K. Patel; J. R. Rygg; J. E. Ralph; J. D. Salmonson; B. K. Spears; P. T. Springer

By increasing the velocity in “high foot” implosions [Dittrich et al., Phys. Rev. Lett. 112, 055002 (2014); Park et al., Phys. Rev. Lett. 112, 055001 (2014); Hurricane et al., Nature 506, 343 (2014); Hurricane et al., Phys. Plasmas 21, 056314 (2014)] on the National Ignition Facility laser, we have nearly doubled the neutron yield and the hotspot pressure as compared to the implosions reported upon last year. The implosion velocity has been increased using a combination of the laser (higher power and energy), the hohlraum (depleted uranium wall material with higher opacity and lower specific heat than gold hohlraums), and the capsule (thinner capsules with less mass). We find that the neutron yield from these experiments scales systematically with a velocity-like parameter of the square root of the laser energy divided by the ablator mass. By connecting this parameter with the inferred implosion velocity ( v), we find that for shots with primary yield >1 × 1015 neutrons, the total yield ∼ v9.4. This incre...

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D. K. Bradley

Lawrence Livermore National Laboratory

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T. Ma

University of Washington

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N. Izumi

Lawrence Livermore National Laboratory

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S. F. Khan

Lawrence Livermore National Laboratory

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D. A. Callahan

Lawrence Livermore National Laboratory

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G. A. Kyrala

Los Alamos National Laboratory

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E. L. Dewald

Lawrence Livermore National Laboratory

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Peter M. Celliers

Lawrence Livermore National Laboratory

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L. Berzak Hopkins

Lawrence Livermore National Laboratory

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R. Tommasini

Lawrence Livermore National Laboratory

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