S. LePape
Lawrence Livermore National Laboratory
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by S. LePape.
Science | 2010
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.
Review of Scientific Instruments | 2012
T. Ma; N. Izumi; R. Tommasini; D. K. Bradley; P. M. Bell; C. Cerjan; S. N. Dixit; T. Döppner; O. S. Jones; J. L. Kline; G. A. Kyrala; O. L. Landen; S. LePape; A. J. Mackinnon; H.-S. Park; P. K. Patel; R. Prasad; J. E. Ralph; S. P. Regan; V. A. Smalyuk; P. T. Springer; L. J. Suter; R. P. J. Town; S. V. Weber; S. H. Glenzer
Accurately assessing and optimizing the implosion performance of inertial confinement fusion capsules is a crucial step to achieving ignition on the NIF. We have applied differential filtering (matched Ross filter pairs) to provide broadband time-integrated absolute x-ray self-emission images of the imploded core of cryogenic layered implosions. This diagnostic measures the temperature- and density-sensitive bremsstrahlung emission and provides estimates of hot spot mass, mix mass, and pressure.
Physics of Plasmas | 2014
J. D. Moody; D. A. Callahan; D. E. Hinkel; Peter A. Amendt; K. L. Baker; D. K. Bradley; Peter M. Celliers; E. L. Dewald; L. Divol; T. Döppner; David C. Eder; M. J. Edwards; O. S. Jones; S. W. Haan; D. Ho; L. B. Hopkins; N. Izumi; D. H. Kalantar; R. L. Kauffman; J. D. Kilkenny; O. L. Landen; Barbara F. Lasinski; S. LePape; T. Ma; B. J. MacGowan; S. A. MacLaren; A. J. Mackinnon; D. Meeker; N. B. Meezan; P. Michel
Advances in hohlraums for inertial confinement fusion at the National Ignition Facility (NIF) were made this past year in hohlraum efficiency, dynamic shape control, and hot electron and x-ray preheat control. Recent experiments are exploring hohlraum behavior over a large landscape of parameters by changing the hohlraum shape, gas-fill, and laser pulse. Radiation hydrodynamic modeling, which uses measured backscatter, shows that gas-filled hohlraums utilize between 60% and 75% of the laser power to match the measured bang-time, whereas near-vacuum hohlraums utilize 98%. Experiments seem to be pointing to deficiencies in the hohlraum (instead of capsule) modeling to explain most of the inefficiency in gas-filled targets. Experiments have begun quantifying the Cross Beam Energy Transfer (CBET) rate at several points in time for hohlraum experiments that utilize CBET for implosion symmetry. These measurements will allow better control of the dynamic implosion symmetry for these targets. New techniques are b...
Physics of Plasmas | 2015
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...
Review of Scientific Instruments | 2013
D. T. Casey; J. A. Frenje; M. Gatu Johnson; F. H. Séguin; C. K. Li; R. D. Petrasso; V. Yu. Glebov; Joseph Katz; J. Magoon; D. D. Meyerhofer; T. C. Sangster; M. J. Shoup; J. Ulreich; R. C. Ashabranner; R. Bionta; A. Carpenter; B. Felker; H. Y. Khater; S. LePape; A. J. Mackinnon; M. McKernan; M. J. Moran; J. R. Rygg; M. Yeoman; R. A. Zacharias; R. J. Leeper; K. Fletcher; M. Farrell; D. Jasion; J. D. Kilkenny
The neutron spectrum produced by deuterium-tritium (DT) inertial confinement fusion implosions contains a wealth of information about implosion performance including the DT yield, ion-temperature, and areal-density. The Magnetic Recoil Spectrometer (MRS) has been used at both the OMEGA laser facility and the National Ignition Facility (NIF) to measure the absolute neutron spectrum from 3 to 30 MeV at OMEGA and 3 to 36 MeV at the NIF. These measurements have been used to diagnose the performance of cryogenic target implosions to unprecedented accuracy. Interpretation of MRS data requires a detailed understanding of the MRS response and background. This paper describes ab initio characterization of the system involving Monte Carlo simulations of the MRS response in addition to the commission experiments for in situ calibration of the systems on OMEGA and the NIF.
Physics of Plasmas | 2015
M. Hohenberger; P. B. Radha; J. F. Myatt; S. LePape; J.A. Marozas; F. J. Marshall; D.T. Michel; S. P. Regan; W. Seka; A. Shvydky; T. C. Sangster; J.W. Bates; R. Betti; T. R. Boehly; M.J. Bonino; D. T. Casey; T.J.B. Collins; R. S. Craxton; J. A. Delettrez; D. H. Edgell; R. Epstein; G. Fiksel; P. Fitzsimmons; J. A. Frenje; D. H. Froula; V.N. Goncharov; D. R. Harding; D. H. Kalantar; Max Karasik; Terrance J. Kessler
To support direct-drive inertial confinement fusion experiments at the National Ignition Facility (NIF) [G. H. Miller, E. I. Moses, and C. R. Wuest, Opt. Eng. 43, 2841 (2004)] in its indirect-drive beam configuration, the polar-direct-drive (PDD) concept [S. Skupsky et al., Phys. Plasmas 11, 2763 (2004)] has been proposed. Ignition in PDD geometry requires direct-drive–specific beam smoothing, phase plates, and repointing the NIF beams toward the equator to ensure symmetric target irradiation. First experiments to study the energetics and preheat in PDD implosions at the NIF have been performed. These experiments utilize the NIF in its current configuration, including beam geometry, phase plates, and beam smoothing. Room-temperature, 2.2-mm-diam plastic shells filled with D2 gas were imploded with total drive energies ranging from ∼500 to 750 kJ with peak powers of 120 to 180 TW and peak on-target irradiances at the initial target radius from 8 × 1014 to 1.2 × 1015 W/cm2. Results from these initial experi...
Physics of Plasmas | 2013
M. Gatu Johnson; D. T. Casey; J. A. Frenje; C. K. Li; F. H. Séguin; R. D. Petrasso; R. C. Ashabranner; R. Bionta; S. LePape; M. McKernan; A. J. Mackinnon; J. D. Kilkenny; J. P. Knauer; T. C. Sangster
For the first time, quantitative measurements of collective fuel velocities in Inertial Confinement Fusion implosions at the National Ignition Facility are reported. Velocities along the line-of-sight (LOS) of the Magnetic Recoil neutron Spectrometer (MRS), positioned close to the equator (73°–324°), were inferred from the measured mean energy of the deuterium-tritium (DT)-primary neutron peak. Substantial mean energy shifts up to 113 ± 16 keV were observed in DT gas-filled exploding-pusher implosions, driven in a polar-direct drive configuration, which corresponds to bulk fuel velocities up to 210 ± 30 km/s. In contrast, only marginal bulk fuel velocities along the MRS LOS were observed in cryogenically layered DT implosions. Integrated analysis of data from a large number of cryogenically layered implosions has recently identified a deficit in achieved hot-spot energy of ∼3 kJ for these implosions [C. Cerjan et al., Phys. Plasmas (2013)]. One hypothesis that could explain this missing energy is a collec...
Physics of Plasmas | 2014
H. F. Robey; Peter M. Celliers; J. D. Moody; J. Sater; T. Parham; B. J. Kozioziemski; R.J. Dylla-Spears; J. S. Ross; S. LePape; J. E. Ralph; M. Hohenberger; E. L. Dewald; L. Berzak Hopkins; J. J. Kroll; B.E. Yoxall; Alex V. Hamza; T. R. Boehly; A. Nikroo; O. L. Landen; M. J. Edwards
Recent advances in shock timing experiments and analysis techniques now enable shock measurements to be performed in cryogenic deuterium-tritium (DT) ice layered capsule implosions on the National Ignition Facility (NIF). Previous measurements of shock timing in inertial confinement fusion implosions [Boehly et al., Phys. Rev. Lett. 106, 195005 (2011); Robey et al., Phys. Rev. Lett. 108, 215004 (2012)] were performed in surrogate targets, where the solid DT ice shell and central DT gas were replaced with a continuous liquid deuterium (D2) fill. These previous experiments pose two surrogacy issues: a material surrogacy due to the difference of species (D2 vs. DT) and densities of the materials used and a geometric surrogacy due to presence of an additional interface (ice/gas) previously absent in the liquid-filled targets. This report presents experimental data and a new analysis method for validating the assumptions underlying this surrogate technique. Comparison of the data with simulation shows good agreement for the timing of the first three shocks, but reveals a considerable discrepancy in the timing of the 4th shock in DT ice layered implosions. Electron preheat is examined as a potential cause of the observed discrepancy in the 4th shock timing.
Physical Review E | 2016
M. Gatu Johnson; J. P. Knauer; C. Cerjan; M. J. Eckart; G. P. Grim; Edward P. Hartouni; R. Hatarik; J. D. Kilkenny; D. H. Munro; D. B. Sayre; B. K. Spears; R. Bionta; E. Bond; J. A. Caggiano; D. A. Callahan; D. T. Casey; T. Döppner; J. A. Frenje; V. Yu. Glebov; O. A. Hurricane; A. L. Kritcher; S. LePape; T. Ma; A. J. Mackinnon; N. B. Meezan; P. K. Patel; R. D. Petrasso; J. E. Ralph; P. T. Springer; C. B. Yeamans
An accurate understanding of burn dynamics in implosions of cryogenically layered deuterium (D) and tritium (T) filled capsules, obtained partly through precision diagnosis of these experiments, is essential for assessing the impediments to achieving ignition at the National Ignition Facility. We present measurements of neutrons from such implosions. The apparent ion temperatures T_{ion} are inferred from the variance of the primary neutron spectrum. Consistently higher DT than DD T_{ion} are observed and the difference is seen to increase with increasing apparent DT T_{ion}. The line-of-sight rms variations of both DD and DT T_{ion} are small, ∼150eV, indicating an isotropic source. The DD neutron yields are consistently high relative to the DT neutron yields given the observed T_{ion}. Spatial and temporal variations of the DT temperature and density, DD-DT differential attenuation in the surrounding DT fuel, and fluid motion variations contribute to a DT T_{ion} greater than the DD T_{ion}, but are in a one-dimensional model insufficient to explain the data. We hypothesize that in a three-dimensional interpretation, these effects combined could explain the results.
Review of Scientific Instruments | 2014
T. Döppner; A. L. Kritcher; Paul Neumayer; D. Kraus; B. Bachmann; S. Burns; R. W. Falcone; S. H. Glenzer; J. Hawreliak; A. House; O. L. Landen; S. LePape; T. Ma; A. Pak; Damian C. Swift
We have designed, built, and successfully fielded a highly efficient and gated Bragg crystal spectrometer for x-ray Thomson scattering measurements on the National Ignition Facility (NIF). It utilizes a cylindrically curved Highly Oriented Pyrolytic Graphite crystal. Its spectral range of 7.4-10 keV is optimized for scattering experiments using a Zn He-α x-ray probe at 9.0 keV or Mo K-shell line emission around 18 keV in second diffraction order. The spectrometer has been designed as a diagnostic instrument manipulator-based instrument for the NIF target chamber at the Lawrence Livermore National Laboratory, USA. Here, we report on details of the spectrometer snout, its novel debris shield configuration and an in situ spectral calibration experiment with a Brass foil target, which demonstrated a spectral resolution of E/ΔE = 220 at 9.8 keV.