Mix and hydrodynamic instabilities on NIF

Several new platforms have been developed to experimentally measure hydrodynamic instabilities in all phases of indirect-drive, inertial confinement fusion implosions on National Ignition Facility. At the ablation front, instability growth of pre-imposed modulations was measured with a face-on, x-ray radiography platform in the linear regime using the Hydrodynamic Growth Radiography (HGR) platform. Modulation growth of "native roughness" modulations and engineering features (fill tubes and capsule support membranes) were measured in conditions relevant to layered DT implosions. A new experimental platform was developed to measure instability growth at the ablator-ice interface. In the deceleration phase of implosions, several experimental platforms were developed to measure both low-mode asymmetries and high-mode perturbations near peak compression with x-ray and nuclear techniques. In one innovative technique, the self-emission from the hot spot was enhanced with argon dopant to "self-backlight" the shell in-flight. To stabilize instability growth, new "adiabat-shaping" techniques were developed using the HGR platform and applied in layered DT implosions.

[1]  O A Hurricane,et al.  High-adiabat high-foot inertial confinement fusion implosion experiments on the national ignition facility. , 2014, Physical review letters.

[2]  Kuppusamy Thayalan,et al.  Radiation Detection and Measurements , 2014 .

[3]  N. Izumi,et al.  Onset of hydrodynamic mix in high-velocity, highly compressed inertial confinement fusion implosions. , 2013, Physical review letters.

[4]  P L Volegov,et al.  Improved Performance of High Areal Density Indirect Drive Implosions at the National Ignition Facility using a Four-Shock Adiabat Shaped Drive. , 2015, Physical review letters.

[5]  O. Landen,et al.  Hydrodynamic instability experiments with three-dimensional modulations at the National Ignition Facility , 2015, High Power Laser Science and Engineering.

[6]  S. Chandrasekhar Hydrodynamic and Hydromagnetic Stability , 1961 .

[7]  A Pak,et al.  2D X-ray radiography of imploding capsules at the national ignition facility. , 2014, Physical review letters.

[8]  V. A. Smalyuk,et al.  Diagnosing and controlling mix in National Ignition Facility implosion experiments a) , 2011 .

[9]  L A Bernstein,et al.  Neutron activation diagnostics at the National Ignition Facility (invited). , 2012, The Review of scientific instruments.

[10]  J. Lindl,et al.  Inertial Confinement Fusion: The Quest for Ignition and Energy Gain Using Indirect Drive , 1998 .

[11]  O. Landen,et al.  First measurements of hydrodynamic instability growth in indirectly driven implosions at ignition-relevant conditions on the National Ignition Facility. , 2014, Physical review letters.

[12]  V. A. Smalyuk,et al.  Hydrodynamic instability growth of three-dimensional, “native-roughness” modulations in x-ray driven, spherical implosions at the National Ignition Facility , 2015 .

[13]  A. MacPhee,et al.  Erratum: First Measurements of Fuel-Ablator Interface Instability Growth in Inertial Confinement Fusion Implosions on the National Ignition Facility [Phys. Rev. Lett. 117, 075002 (2016)]. , 2016, Physical review letters.

[14]  J. Meyer-ter-Vehn,et al.  The physics of inertial fusion - Hydrodynamics, dense plasma physics, beam-plasma interaction , 2004 .

[15]  D. Clark,et al.  Design of indirectly driven, high-compression Inertial Confinement Fusion implosions with improved hydrodynamic stability using a 4-shock adiabat-shaped drive , 2015 .

[16]  V. A. Smalyuk,et al.  Performance of indirectly driven capsule implosions on the National Ignition Facility using adiabat-shaping , 2016 .

[17]  D S Clark,et al.  X-ray shadow imprint of hydrodynamic instabilities on the surface of inertial confinement fusion capsules by the fuel fill tube. , 2017, Physical review. E.

[18]  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.

[19]  O. Landen,et al.  An in-flight radiography platform to measure hydrodynamic instability growth in inertial confinement fusion capsules at the National Ignition Facility , 2014 .

[20]  Haan Onset of nonlinear saturation for Rayleigh-Taylor growth in the presence of a full spectrum of modes. , 1989, Physical review. A, General physics.

[21]  D. Clark,et al.  A survey of pulse shape options for a revised plastic ablator ignition design , 2014 .

[22]  L. Pickworth,et al.  Measurement of Hydrodynamic Growth near Peak Velocity in an Inertial Confinement Fusion Capsule Implosion using a Self-Radiography Technique. , 2016, Physical review letters.

[23]  D. K. Bradley,et al.  Tent-induced perturbations on areal density of implosions at the National Ignition Facilitya) , 2015 .

[24]  D. Clark,et al.  Simulations and experiments of the growth of the “tent” perturbation in NIF ignition implosions , 2016 .

[25]  L. Pickworth,et al.  Measuring shell-$\rho $R perturbations in NIF capsule implosions near peak velocity , 2013 .

[26]  V. A. Smalyuk,et al.  Experimental results of radiation-driven, layered deuterium-tritium implosions with adiabat-shaped drives at the National Ignition Facility , 2016 .

[27]  S. Haan Instability Growth Seeded by Oxygen in CH Shells on the National Ignition Facility , 2014 .

[28]  L. Pickworth,et al.  Hydrodynamic instability growth and mix experiments at the National Ignition Facilitya) , 2014 .

[29]  O. Landen,et al.  Measurements of an ablator-gas atomic mix in indirectly driven implosions at the National Ignition Facility. , 2014, Physical review letters.