Time-Resolved Fuel Density Profiles of the Stagnation Phase of Indirect-Drive Inertial Confinement Implosions.

The implosion efficiency in inertial confinement fusion depends on the degree of stagnated fuel compression, density uniformity, sphericity, and minimum residual kinetic energy achieved. Compton scattering-mediated 50-200 keV x-ray radiographs of indirect-drive cryogenic implosions at the National Ignition Facility capture the dynamic evolution of the fuel as it goes through peak compression, revealing low-mode 3D nonuniformities and thicker fuel with lower peak density than simulated. By differencing two radiographs taken at different times during the same implosion, we also measure the residual kinetic energy not transferred to the hot spot and quantify its impact on the implosion performance.

[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 .