Time-Resolved Fuel Density Profiles of the Stagnation Phase of Indirect-Drive Inertial Confinement Implosions.
暂无分享,去创建一个
L. Divol | O. Landen | J. Holder | P. Di Nicola | D. Kalantar | R. Lowe-Webb | R. Tommasini | J. Milovich | A. Nikroo | M. Herrmann | A. Kemp | N. Masters | P. Wegner | M. Bowers | W. Williams | C. Widmayer | D. Alessi | J. Heebner | M. Hermann | P. Volegov | D. Fittinghoff | N. Izumi | S. Hatchett | K. LaFortune | R. Wallace | D. Bradley | A. Conder | A. Mackinnon | J. Kroll | S. Bhandarkar | W. Hsing | T. Kohut | C. Walters | M. Edwards | M. Prantil | D. Martinez | M. Hamamoto | D. Homoelle | J. Lawson | L. Pelz | R. Sigurdsson | J. Di Nicola | L. B. Berzak Hopkins | C. Iglesias | G. Gururangan | S. Vonhof | K. Youngblood | D. Holunga | J. Park | M. Schoff | D. Hargrove | T. Zobrist | M. Mauldin | E. Hartouni | G. Hall | S. Ayers | S. Herriot | J. Okui | K. Lafortune | J. Kroll
[1] V. J. Hernandez,et al. High-energy (>70 keV) x-ray conversion efficiency measurement on the ARC laser at the National Ignition Facility , 2017 .
[2] P. B. Radha,et al. Impact of three-dimensional hot-spot flow asymmetry on ion-temperature measurements in inertial confinement fusion experiments , 2018, Physics of Plasmas.
[3] D. K. Bradley,et al. Metrics for long wavelength asymmetries in inertial confinement fusion implosions on the National Ignition Facility , 2014 .
[4] Glebov,et al. A new neutron time-of-flight detector to measure the MeV neutron spectrum at the National Ignition Facility and its applications , 2013 .
[5] R. Betti,et al. The Physics of Long- and Intermediate-Wavelength Asymmetries of the Hot Spot , 2017 .
[6] Jeffrey A. Koch,et al. Application of imaging plates to x-ray imaging and spectroscopy in laser plasma experiments (invited) , 2006 .
[7] Y. P. Opachich,et al. Measuring x-ray burn history with the Streaked Polar Instrumentation for Diagnosing Energetic Radiation (SPIDER) at the National Ignition Facility (NIF) , 2012, Other Conferences.
[8] Steven W. Haan,et al. A comparison of three-dimensional multimode hydrodynamic instability growth on various National Ignition Facility capsule designs with HYDRA simulations , 1998 .
[9] L A Bernstein,et al. Enhanced NIF neutron activation diagnostics. , 2012, The Review of scientific instruments.
[10] O. Klein,et al. Über die Streuung von Strahlung durch freie Elektronen nach der neuen relativistischen Quantendynamik von Dirac , 1929 .
[11] Masakatsu Murakami,et al. Indirectly driven targets for inertial confinement fusion , 1991 .
[12] J. Lindl. Development of the indirect‐drive approach to inertial confinement fusion and the target physics basis for ignition and gain , 1995 .
[13] R W Falcone,et al. Absolute Equation-of-State Measurement for Polystyrene from 25 to 60 Mbar Using a Spherically Converging Shock Wave. , 2018, Physical review letters.
[14] J. Meyer-ter-Vehn,et al. Inertial Confinement Fusion , 1998 .
[15] Karen S. Anderson,et al. Thermonuclear ignition in inertial confinement fusion and comparison with magnetic confinement , 2010 .
[16] L. J. Atherton,et al. The experimental plan for cryogenic layered target implosions on the National Ignition Facility--The inertial confinement approach to fusion , 2011 .
[17] O. Landen,et al. Azimuthal Drive Asymmetry in Inertial Confinement Fusion Implosions on the National Ignition Facility. , 2020, Physical review letters.
[18] C R Danly,et al. Neutron source reconstruction from pinhole imaging at National Ignition Facility. , 2014, The Review of scientific instruments.
[19] Nick Schenkel,et al. Injection laser system for Advanced Radiographic Capability using chirped pulse amplification on the National Ignition Facility. , 2019, Applied optics.
[20] J. Chittenden,et al. Density determination of the thermonuclear fuel region in inertial confinement fusion implosions , 2020 .
[21] Gilbert W. Collins,et al. In-flight observations of low-mode ρR asymmetries in NIF implosionsa) , 2015 .
[22] D. Turnbull,et al. Indirect drive ignition at the National Ignition Facility , 2016 .
[23] O. Landen,et al. Fluence-compensated down-scattered neutron imaging using the neutron imaging system at the National Ignition Facility. , 2016, The Review of scientific instruments.
[24] L. Divol,et al. Beyond alpha-heating: driving inertially confined fusion implosions toward a burning-plasma state on the National Ignition Facility , 2018, Plasma Physics and Controlled Fusion.
[25] J. Kilkenny,et al. Mode 1 drive asymmetry in inertial confinement fusion implosions on the National Ignition Facility , 2014 .
[26] J. R. Rygg,et al. Symmetry control of an indirectly driven high-density-carbon implosion at high convergence and high velocity , 2017 .
[27] L. Divol,et al. Increasing stagnation pressure and thermonuclear performance of inertial confinement fusion capsules by the introduction of a high-Z dopant , 2018, Physics of Plasmas.
[28] Edward I. Moses,et al. The National Ignition Facility: enabling fusion ignition for the 21st century , 2004 .
[29] D. K. Bradley,et al. Short pulse, high resolution, backlighters for point projection high-energy radiography at the National Ignition Facility , 2017 .
[30] O. Landen,et al. View factor estimation of hot spot velocities in inertial confinement fusion implosions at the National Ignition Facility , 2020 .
[31] L. J. Atherton,et al. Implosion dynamics measurements at the National Ignition Facility , 2012 .
[32] C. Sorce,et al. Development of Compton radiography of inertial confinement fusion implosionsa) , 2011 .
[33] B. Spears,et al. Using multiple neutron time of flight detectors to determine the hot spot velocity. , 2018, The Review of scientific instruments.
[34] R. B. Ehrlich,et al. Nuclear imaging of the fuel assembly in ignition experimentsa) , 2012 .