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Dive into the research topics where C. B. Yeamans is active.

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Featured researches published by C. B. Yeamans.


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...


Review of Scientific Instruments | 2012

Neutron spectrometry--an essential tool for diagnosing implosions at the National Ignition Facility (invited).

M. Gatu Johnson; J. A. Frenje; D. T. Casey; C. K. Li; F. H. Séguin; R. D. Petrasso; R. C. Ashabranner; R. Bionta; D. L. Bleuel; E. Bond; J. A. Caggiano; A. Carpenter; C. Cerjan; T. J. Clancy; T. Doeppner; M. J. Eckart; M. J. Edwards; S. Friedrich; S. H. Glenzer; S. W. Haan; Edward P. Hartouni; R. Hatarik; S. P. Hatchett; O. S. Jones; G. A. Kyrala; S. Le Pape; R. A. Lerche; O. L. Landen; T. Ma; A. J. Mackinnon

DT neutron yield (Y(n)), ion temperature (T(i)), and down-scatter ratio (dsr) determined from measured neutron spectra are essential metrics for diagnosing the performance of inertial confinement fusion (ICF) implosions at the National Ignition Facility (NIF). A suite of neutron-time-of-flight (nTOF) spectrometers and a magnetic recoil spectrometer (MRS) have been implemented in different locations around the NIF target chamber, providing good implosion coverage and the complementarity required for reliable measurements of Y(n), T(i), and dsr. From the measured dsr value, an areal density (ρR) is determined through the relationship ρR(tot) (g∕cm(2)) = (20.4 ± 0.6) × dsr(10-12 MeV). The proportionality constant is determined considering implosion geometry, neutron attenuation, and energy range used for the dsr measurement. To ensure high accuracy in the measurements, a series of commissioning experiments using exploding pushers have been used for in situ calibration of the as-built spectrometers, which are now performing to the required accuracy. Recent data obtained with the MRS and nTOFs indicate that the implosion performance of cryogenically layered DT implosions, characterized by the experimental ignition threshold factor (ITFx), which is a function of dsr (or fuel ρR) and Y(n), has improved almost two orders of magnitude since the first shot in September, 2010.


Inorganic Chemistry | 2009

Reaction Sequence and Kinetics of Uranium Nitride Decomposition

G. W. Chinthaka Silva; C. B. Yeamans; Alfred P. Sattelberger; Thomas Hartmann; Gary S. Cerefice; Kenneth R. Czerwinski

The reaction mechanism and kinetics of the thermal decomposition of uranium dinitride/uranium sesquinitride to uranium mononitride under inert atmosphere at elevated temperature were studied. An increase in the lattice parameter of the UN(2)/alpha-U(2)N(3) phase was observed as the reaction temperature increased, corresponding to a continuous removal of nitrogen. Electron density calculations for these two compounds using XRD powder patterns of the samples utilizing charge-flipping technique were performed for the first time to visualize the decrease in nitrogen level as a function of temperature. Complete decomposition of UN(2) into alpha-U(2)N(3) at 675 degrees C and the UN formation after a partial decomposition of alpha-U(2)N(3) at 975 degrees C were also identified in this study. The activation energy for the decomposition of the UN(2)/alpha-U(2)N(3) phase into UN, 423.8 +/- 0.3 kJ/mol (101.3 kcal/mol), was determined under an inert argon atmosphere and is reported here experimentally for the first time.


Physics of Plasmas | 2014

Hydrodynamic instability growth and mix experiments at the National Ignition Facilitya)

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...


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.


Physics of Plasmas | 2016

Performance of indirectly driven capsule implosions on the National Ignition Facility using adiabat-shaping

H. F. Robey; V. A. Smalyuk; J. L. Milovich; T. Döppner; D. T. Casey; K. L. Baker; J. L. Peterson; B. Bachmann; L. Berzak Hopkins; E. Bond; J. A. Caggiano; D. A. Callahan; Peter M. Celliers; C. Cerjan; D. S. Clark; S. Dixit; M. J. Edwards; N. Gharibyan; S. W. Haan; B. A. Hammel; Alex V. Hamza; R. Hatarik; O. A. Hurricane; K. S. Jancaitis; O. S. Jones; G.D. Kerbel; J. J. Kroll; K. N. Lafortune; O. L. Landen; T. Ma

A series of indirectly driven capsule implosions has been performed on the National Ignition Facility to assess the relative contributions of ablation-front instability growth vs. fuel compression on implosion performance. Laser pulse shapes for both low and high-foot pulses were modified to vary ablation-front growth and fuel adiabat, separately and controllably. Three principal conclusions are drawn from this study: (1) It is shown that reducing ablation-front instability growth in low-foot implosions results in a substantial (3-10X) increase in neutron yield with no loss of fuel compression. (2) It is shown that reducing the fuel adiabat in high-foot implosions results in a significant (36%) increase in fuel compression together with a small (10%) increase in neutron yield. (3) Increased electron preheat at higher laser power in high-foot implosions, however, appears to offset the gain in compression achieved by adiabat-shaping at lower power. These results taken collectively bridge the space between t...


Physics of Plasmas | 2015

First results of radiation-driven, layered deuterium-tritium implosions with a 3-shock adiabat-shaped drive at the National Ignition Facility

V. A. Smalyuk; H. F. Robey; T. Döppner; O. S. Jones; J. L. Milovich; B. Bachmann; K. L. Baker; L. Berzak Hopkins; E. Bond; D. A. Callahan; D. T. Casey; Peter M. Celliers; C. Cerjan; D. S. Clark; S. Dixit; M. J. Edwards; E. Giraldez; S. W. Haan; Alex V. Hamza; M. Hohenberger; D. Hoover; O. A. Hurricane; K. S. Jancaitis; J. J. Kroll; K. N. Lafortune; O. L. Landen; B. J. MacGowan; A. G. MacPhee; A. Nikroo; A. Pak

Radiation-driven, layered deuterium-tritium plastic capsule implosions were carried out using a new, 3-shock “adiabat-shaped” drive on the National Ignition Facility. The purpose of adiabat shaping is to use a stronger first shock, reducing hydrodynamic instability growth in the ablator. The shock can decay before reaching the deuterium-tritium fuel leaving it on a low adiabat and allowing higher fuel compression. The fuel areal density was improved by ∼25% with this new drive compared to similar “high-foot” implosions, while neutron yield was improved by more than 4 times, compared to “low-foot” implosions driven at the same compression and implosion velocity.


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.


Review of Scientific Instruments | 2012

Enhanced NIF neutron activation diagnostics.

C. B. Yeamans; D. L. Bleuel; Lee Allen Bernstein

The NIF neutron activation diagnostic suite relies on removable activation samples, leading to operational inefficiencies and a fundamental lower limit on the half-life of the activated product that can be observed. A neutron diagnostic system measuring activation of permanently installed samples could remove these limitations and significantly enhance overall neutron diagnostic capabilities. The physics and engineering aspects of two proposed systems are considered: one measuring the (89)Zr/(89 m)Zr isomer ratio in the existing Zr activation medium and the other using potassium zirconate as the activation medium. Both proposed systems could improve the signal-to-noise ratio of the current system by at least a factor of 5 and would allow independent measurement of fusion core velocity and fuel areal density.


Review of Scientific Instruments | 2012

Measuring the absolute deuterium-tritium neutron yield using the magnetic recoil spectrometer at OMEGA and the NIF.

D. T. Casey; J. A. Frenje; M. Gatu Johnson; F. H. Séguin; C. K. Li; R. D. Petrasso; V. Yu. Glebov; Joseph Katz; J. P. Knauer; D. D. Meyerhofer; T. C. Sangster; R. Bionta; D. L. Bleuel; T. Döppner; S. H. Glenzer; Edward P. Hartouni; S. P. Hatchett; S. Le Pape; T. Ma; A. J. Mackinnon; M. McKernan; M. J. Moran; Eric K. Moses; H.-S. Park; J. E. Ralph; B. A. Remington; V. A. Smalyuk; C. B. Yeamans; J. L. Kline; G. A. Kyrala

A magnetic recoil spectrometer (MRS) has been installed and extensively used on OMEGA and the National Ignition Facility (NIF) for measurements of the absolute neutron spectrum from inertial confinement fusion implosions. From the neutron spectrum measured with the MRS, many critical implosion parameters are determined including the primary DT neutron yield, the ion temperature, and the down-scattered neutron yield. As the MRS detection efficiency is determined from first principles, the absolute DT neutron yield is obtained without cross-calibration to other techniques. The MRS primary DT neutron measurements at OMEGA and the NIF are shown to be in excellent agreement with previously established yield diagnostics on OMEGA, and with the newly commissioned nuclear activation diagnostics on the NIF.

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D. T. Casey

Lawrence Livermore National Laboratory

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T. Ma

University of Washington

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R. Hatarik

Lawrence Livermore National Laboratory

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D. A. Callahan

Lawrence Livermore National Laboratory

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J. A. Caggiano

Lawrence Livermore National Laboratory

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J. A. Frenje

Massachusetts Institute of Technology

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R. Bionta

Lawrence Livermore National Laboratory

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L. Berzak Hopkins

Lawrence Livermore National Laboratory

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D. B. Sayre

Lawrence Livermore National Laboratory

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O. A. Hurricane

Lawrence Livermore National Laboratory

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