M. A. Barrios
University of Rochester
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Featured researches published by M. A. Barrios.
Physics of Plasmas | 2010
M. A. Barrios; D.G. Hicks; T. R. Boehly; D. E. Fratanduono; Jon H. Eggert; Peter M. Celliers; G. W. Collins; D. D. Meyerhofer
The equation of state (EOS) of polystyrene and polypropylene were measured using laser-driven shock waves with pressures from 1 to 10 Mbar. Precision data resulting from the use of α-quartz as an impedance-matching (IM) standard tightly constrains the EOS of these hydrocarbons, even with the inclusion of systematic errors inherent to IM. The temperature at these high pressures was measured, which, combined with kinematic measurements, provide a complete shock EOS. Both hydrocarbons were observed to reach similar compressions and temperatures as a function of pressure. The materials were observed to transition from transparent insulators to reflecting conductors at pressures of 1 to 2 Mbar.
Physics of Plasmas | 2012
S. P. Regan; R. Epstein; B. A. Hammel; L. J. Suter; J. E. Ralph; Howard A. Scott; M. A. Barrios; D. K. Bradley; D. A. Callahan; C. Cerjan; G. W. Collins; S. Dixit; T. Doeppner; M. J. Edwards; D. R. Farley; S. Glenn; S. H. Glenzer; I. E. Golovkin; S. W. Haan; Alex V. Hamza; Damien G. Hicks; N. Izumi; J. D. Kilkenny; J. L. Kline; G. A. Kyrala; O. L. Landen; T. Ma; J. J. MacFarlane; R. C. Mancini; R. L. McCrory
Ignition of an inertial confinement fusion (ICF) target depends on the formation of a central hot spot with sufficient temperature and areal density. Radiative and conductive losses from the hot spot can be enhanced by hydrodynamic instabilities. The concentric spherical layers of current National Ignition Facility (NIF) ignition targets consist of a plastic ablator surrounding a thin shell of cryogenic thermonuclear fuel (i.e., hydrogen isotopes), with fuel vapor filling the interior volume [S. W. Haan et al., Phys. Plasmas 18, 051001 (2011)]. The Rev. 5 ablator is doped with Ge to minimize preheat of the ablator closest to the DT ice caused by Au M-band emission from the hohlraum x-ray drive [D. S. Clark et al., Phys. Plasmas 17, 052703 (2010)]. Richtmyer–Meshkov and Rayleigh–Taylor hydrodynamic instabilities seeded by high-mode (50<l<200) ablator-surface perturbations can cause Ge-doped ablator to mix into the interior of the shell at the end of the acceleration phase [B. A. Hammel et al., Phys. Plasma...
Physics of Plasmas | 2014
V. A. Smalyuk; M. A. Barrios; J. A. Caggiano; D. T. Casey; C. Cerjan; D. S. Clark; M. J. Edwards; J. A. Frenje; M. Gatu-Johnson; Vladimir Yu. Glebov; G. P. Grim; S. W. Haan; B. A. Hammel; Alex V. Hamza; D. Hoover; W. W. Hsing; O. A. Hurricane; J. D. Kilkenny; J. L. Kline; J. P. Knauer; J. J. Kroll; O. L. Landen; J. D. Lindl; T. Ma; J. McNaney; M. Mintz; A. S. Moore; A. Nikroo; T. Parham; J. L. Peterson
Hydrodynamic instability growth and its effects on implosion performance were studied at the National Ignition Facility [G. H. Miller, E. I. Moses, and C. R. Wuest, Opt. Eng. 443, 2841 (2004)]. Implosion performance and mix have been measured at peak compression using plastic shells filled with tritium gas and containing embedded localized carbon-deuterium diagnostic layers in various locations in the ablator. Neutron yield and ion temperature of the deuterium-tritium fusion reactions were used as a measure of shell-gas mix, while neutron yield of the tritium-tritium fusion reaction was used as a measure of implosion performance. The results have indicated that the low-mode hydrodynamic instabilities due to surface roughness were the primary culprits for yield degradation, with atomic ablator-gas mix playing a secondary role. In addition, spherical shells with pre-imposed 2D modulations were used to measure instability growth in the acceleration phase of the implosions. The capsules were imploded using ig...
Journal of Applied Physics | 2011
D. E. Fratanduono; T. R. Boehly; Peter M. Celliers; M. A. Barrios; Jon H. Eggert; Raymond F. Smith; D. G. Hicks; G. W. Collins; D. D. Meyerhofer
The instantaneous scaling of ablation pressure to laser intensity is directly inferred for ramp compression of diamond targets irradiated by 351-nm light. Continuously increasing pressure profiles from 100 to 970 GPa are produced by direct-drive laser ablation at intensities up to 7 × 1013 W/cm2. The free-surface velocity on the rear of the target is used to directly infer the instantaneous ablation-pressure profile at the front of the target. The laser intensity on target is determined by laser power measurements and fully characterized laser spots. The ablation pressure is found to depend on the laser intensity as P(GPa)=42(±3)[I(TW/cm2)]0.71(±0.01).
Review of Scientific Instruments | 2012
N. Izumi; T. Ma; M. A. Barrios; L. R. Benedetti; D. A. Callahan; C. Cerjan; John Edwards; S. Glenn; S. H. Glenzer; J. D. Kilkenny; J. L. Kline; G. A. Kyrala; O. L. Landen; S. P. Regan; P. T. Springer; L. J. Suter; R. Tommasini; R. P. J. Town; A. J. Mackinnon; P. M. Bell; D. K. Bradley
The electron and ion temperatures of the imploded core plasma are two of the most important metrics of inertial confinement fusion experiments. We have developed a technique for inferring electron temperatures from the contrast of x-ray images observed through a group of x-ray filters. Generally, the plasma electron temperature exhibits spatial and temporal variations, so time-averaged and time-resolved measurements are expected to yield somewhat different results. By analyzing the intensity of images observed with both a time-integrated detector (imaging plates) and a time-resolved detector (gated micro-channel plate), we found the electron temperature observed from x-ray images to be systematically higher than the ion temperature inferred from fusion neutron spectroscopy.
Journal of Applied Physics | 2012
M. A. Barrios; T. R. Boehly; D. G. Hicks; D. E. Fratanduono; J. H. Eggert; G. W. Collins; D. D. Meyerhofer
A large uncertainty in the design of ignition capsules for use in the National Ignition Campaign (NIC) is the ablator equation of state. In this article, we report equation-of-state measurements for two candidate NIC ablator materials, glow-discharge polymer (GDP), and germanium-doped GDP. These materials were driven to pressures of 1 to 12 Mbar using laser-driven shock waves. Hugoniot measurements were obtained using the impedance matching technique with an α-quartz standard. This article presents the first kinematic measurements in the high-pressure fluid regime for these materials, which show to be in close agreement with Livermore equation-of-state model predictions.
Review of Scientific Instruments | 2012
M. J. Haugh; S. P. Regan; K. D. Jacoby; P. W. Ross; J. Magoon; M. A. Barrios; J. Emig; M. J. Shoup; K. B. Fournier
The elliptically curved pentaerythritol (PET) crystals used in the Supersnout 2 x-ray spectrometer on the National Ignition Facility at Lawrence Livermore National Laboratory have been calibrated photometrically in the range of 5.5-16 keV. The elliptical geometry provides broad spectral coverage and minimizes the degradation of spectral resolution due to the finite source size. The reflectivity curve of the crystals was measured using a x-ray line source. The integrated reflectivity (R(I)) and width of its curve (ΔΘ) were the measurements of major interest. The former gives the spectrometer throughput, and the latter gives the spectrometer resolving power. Both parameters are found to vary considerably with the radius of curvature of the crystal and with spectral energy. The results are attributed to an enhanced mosaic effect due to the increase in curvature. There are also contributions from the crystal cleaving and gluing processes.
Journal of Applied Physics | 2011
D. E. Fratanduono; Jon H. Eggert; T. R. Boehly; M. A. Barrios; D. D. Meyerhofer; B. J. Jensen; G. W. Collins
A new technique to measure the refractive index of shocked materials is reported. The arrival of a transparent shock at the free surface of an optical window generates a discontinuity in the observed interferometry record. In this work, we show that the magnitude of that discontinuity is simply defined by the shock velocity, the shocked refractive, and the free-surface velocity. This new technique, to measure the high-pressure refractive index of a transparent material, is demonstrated.
Physics of Plasmas | 2015
A. Zylstra; J. A. Frenje; F. H. Séguin; J. R. Rygg; A. L. Kritcher; M. Rosenberg; H. G. Rinderknecht; Damien G. Hicks; S. Friedrich; R. Bionta; N. B. Meezan; R.E. Olson; J. Atherton; M. A. Barrios; P. M. Bell; R. Benedetti; L. Berzak Hopkins; R. Betti; D. K. Bradley; D. A. Callahan; D. T. Casey; G. W. Collins; E. L. Dewald; S. N. Dixit; T. Döppner; M. J. Edwards; M. Gatu Johnson; S. Glenn; G. P. Grim; S. P. Hatchett
Charged-particle spectroscopy is used to assess implosion symmetry in ignition-scale indirect-drive implosions for the first time. Surrogate D3He gas-filled implosions at the National Ignition Facility produce energetic protons via D+3He fusion that are used to measure the implosion areal density (ρR) at the shock-bang time. By using protons produced several hundred ps before the main compression bang, the implosion is diagnosed in-flight at a convergence ratio of 3–5 just prior to peak velocity. This isolates acceleration-phase asymmetry growth. For many surrogate implosions, proton spectrometers placed at the north pole and equator reveal significant asymmetries with amplitudes routinely ≳10%, which are interpreted as l=2 Legendre modes. With significant expected growth by stagnation, it is likely that these asymmetries would degrade the final implosion performance. X-ray self-emission images at stagnation show asymmetries that are positively correlated with the observed in-flight asymmetries and compar...
Review of Scientific Instruments | 2014
J. E. Field; J. R. Rygg; M. A. Barrios; L. R. Benedetti; T. Döppner; N. Izumi; O. S. Jones; S. F. Khan; T. Ma; S. R. Nagel; A. Pak; R. Tommasini; D. K. Bradley; R. P. J. Town
Two-dimensional radiographs of imploding fusion capsules are obtained at the National Ignition Facility by projection through a pinhole array onto a time-gated framing camera. Parallax among images in the image array makes it possible to distinguish contributions from the capsule and from the backlighter, permitting correction of backlighter non-uniformities within the capsule radiograph. Furthermore, precise determination of the imaging system geometry and implosion velocity enables combination of multiple images to reduce signal-to-noise and discover new capsule features.