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Dive into the research topics where R. Bionta is active.

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Featured researches published by R. Bionta.


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.


Nuclear Fusion | 2013

Diagnosing implosion performance at the National Ignition Facility (NIF) by means of neutron spectrometry

J. A. Frenje; R. Bionta; E. Bond; J. A. Caggiano; D. T. Casey; Charles Cerjan; J. Edwards; M. J. Eckart; D. N. Fittinghoff; S. Friedrich; V. Yu. Glebov; S. H. Glenzer; Gary P. Grim; S. W. Haan; R. Hatarik; S. P. Hatchett; M. Gatu Johnson; O. S. Jones; J. D. Kilkenny; J. P. Knauer; O. L. Landen; R. J. Leeper; S. Le Pape; R. A. Lerche; C. K. Li; A. J. Mackinnon; J. M. McNaney; F. E. Merrill; M. J. Moran; David H. Munro

The neutron spectrum from a cryogenically layered deuterium?tritium (dt) implosion at the National Ignition Facility (NIF) provides essential information about the implosion performance. From the measured primary-neutron spectrum (13?15?MeV), yield (Yn) and hot-spot ion temperature (Ti) are determined. From the scattered neutron yield (10?12?MeV) relative to Yn, the down-scatter ratio, and the fuel areal density (?R) are determined. These implosion parameters have been diagnosed to an unprecedented accuracy with a suite of neutron-time-of-flight spectrometers and a magnetic recoil spectrometer implemented in various locations around the NIF target chamber. This provides good implosion coverage and excellent measurement complementarity required for reliable measurements of Yn, Ti and ?R, in addition to ?R asymmetries. The data indicate that the implosion performance, characterized by the experimental ignition threshold factor, has improved almost two orders of magnitude since the first shot taken in September 2010. ?R values greater than 1?g?cm?2 are readily achieved. Three-dimensional semi-analytical modelling and numerical simulations of the neutron-spectrometry data, as well as other data for the hot spot and main fuel, indicate that a maximum hot-spot pressure of ?150?Gbar has been obtained, which is almost a factor of two from the conditions required for ignition according to simulations. Observed Yn are also 3?10 times lower than predicted. The conjecture is that the observed pressure and Yn deficits are partly explained by substantial low-mode ?R asymmetries, which may cause inefficient conversion of shell kinetic energy to hot-spot thermal energy at stagnation.


Physics of Plasmas | 2015

Cryogenic tritium-hydrogen-deuterium and deuterium-tritium layer implosions with high density carbon ablators in near-vacuum hohlraums

N. B. Meezan; L. Berzak Hopkins; S. Le Pape; L. Divol; A. J. Mackinnon; T. Döppner; D. Ho; O. S. Jones; S. F. Khan; T. Ma; J. L. Milovich; A. Pak; J. S. Ross; C. A. Thomas; L.R. Benedetti; D. K. Bradley; Peter M. Celliers; D. S. Clark; J. E. Field; S. W. Haan; N. Izumi; G. A. Kyrala; J. D. Moody; P. K. Patel; J. E. Ralph; J. R. Rygg; S. M. Sepke; B. K. Spears; R. Tommasini; R. P. J. Town

High Density Carbon (or diamond) is a promising ablator material for use in near-vacuum hohlraums, as its high density allows for ignition designs with laser pulse durations of <10 ns. A series of Inertial Confinement Fusion (ICF) experiments in 2013 on the National Ignition Facility [Moses et al., Phys. Plasmas 16, 041006 (2009)] culminated in a deuterium-tritium (DT) layered implosion driven by a 6.8 ns, 2-shock laser pulse. This paper describes these experiments and comparisons with ICF design code simulations. Backlit radiography of a tritium-hydrogen-deuterium (THD) layered capsule demonstrated an ablator implosion velocity of 385 km/s with a slightly oblate hot spot shape. Other diagnostics suggested an asymmetric compressed fuel layer. A streak camera-based hot spot self-emission diagnostic (SPIDER) showed a double-peaked history of the capsule self-emission. Simulations suggest that this is a signature of low quality hot spot formation. Changes to the laser pulse and pointing for a subsequent DT i...


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...


Review of Scientific Instruments | 2013

The magnetic recoil spectrometer for measurements of the absolute neutron spectrum 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. 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.


Review of Scientific Instruments | 2012

A novel particle time of flight diagnostic for measurements of shock- and compression-bang times in D3He and DT implosions at the NIF

H. G. Rinderknecht; M. Gatu Johnson; A. Zylstra; N. Sinenian; M. Rosenberg; J. A. Frenje; C. Waugh; C. K. Li; F. H. Séguin; R. D. Petrasso; J. R. Rygg; J. R. Kimbrough; A. G. MacPhee; G. W. Collins; Damien G. Hicks; A. J. Mackinnon; P. Bell; R. Bionta; Thomas E. Clancy; R. A. Zacharias; T. Döppner; H.-S. Park; S. LePape; O. L. Landen; N. B. Meezan; E. I. Moses; V. U. Glebov; C. Stoeckl; T. C. Sangster; R.E. Olson

The particle-time-of-flight (pTOF) diagnostic, fielded alongside a wedge range-filter (WRF) proton spectrometer, will provide an absolute timing for the shock-burn weighted ρR measurements that will validate the modeling of implosion dynamics at the National Ignition Facility (NIF). In the first phase of the project, pTOF has recorded accurate bang times in cryogenic DT, DT exploding pusher, and D(3)He implosions using DD or DT neutrons with an accuracy better than ±70 ps. In the second phase of the project, a deflecting magnet will be incorporated into the pTOF design for simultaneous measurements of shock- and compression-bang times in D(3)He-filled surrogate implosions using D(3)He protons and DD-neutrons, respectively.


Review of Scientific Instruments | 2012

Charged-particle spectroscopy for diagnosing shock &#0961;R 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.


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.


Physics of Plasmas | 2013

Measurements of collective fuel velocities in deuterium-tritium exploding pusher and cryogenically layered deuterium-tritium implosions on the NIF

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...


Physical Review E | 2016

Indications of flow near maximum compression in layered deuterium-tritium implosions at the National Ignition Facility.

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.

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J. A. Frenje

Massachusetts Institute of Technology

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D. T. Casey

Lawrence Livermore National Laboratory

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R. D. Petrasso

Massachusetts Institute of Technology

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F. H. Séguin

Massachusetts Institute of Technology

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C. K. Li

Massachusetts Institute of Technology

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M. Gatu Johnson

Massachusetts Institute of Technology

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A. J. Mackinnon

Lawrence Livermore National Laboratory

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J. D. Kilkenny

Lawrence Livermore National Laboratory

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O. L. Landen

Lawrence Livermore National Laboratory

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H. G. Rinderknecht

Lawrence Livermore National Laboratory

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