Adiabat-shaping in indirect drive inertial confinement fusion

Adiabat-shaping techniques were investigated in indirect drive inertial confinement fusion experiments on the National Ignition Facility as a means to improve implosion stability, while still maintaining a low adiabat in the fuel. Adiabat-shaping was accomplished in these indirect drive experiments by altering the ratio of the picket and trough energies in the laser pulse shape, thus driving a decaying first shock in the ablator. This decaying first shock is designed to place the ablation front on a high adiabat while keeping the fuel on a low adiabat. These experiments were conducted using the keyhole experimental platform for both three and four shock laser pulses. This platform enabled direct measurement of the shock velocities driven in the glow-discharge polymer capsule and in the liquid deuterium, the surrogate fuel for a DT ignition target. The measured shock velocities and radiation drive histories are compared to previous three and four shock laser pulses. This comparison indicates that in the ca...

[1]  Gilbert W. Collins,et al.  Shock-induced transformation of liquid deuterium into a metallic fluid , 2000, Physical review letters.

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

[3]  E. Meshkov Instability of the interface of two gases accelerated by a shock wave , 1969 .

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

[5]  Gilbert W. Collins,et al.  Equation of state of CH1.36: First-principles molecular dynamics simulations and shock-and-release wave speed measurements , 2012 .

[6]  Steven W. Haan,et al.  Three-dimensional HYDRA simulations of National Ignition Facility targets , 2001 .

[7]  J. Lindl Development of the indirect‐drive approach to inertial confinement fusion and the target physics basis for ignition and gain , 1995 .

[8]  Gilbert W. Collins,et al.  Precision equation-of-state measurements on National Ignition Facility ablator materials from 1 to 12 Mbar using laser-driven shock waves , 2012 .

[9]  G. Taylor The instability of liquid surfaces when accelerated in a direction perpendicular to their planes. I , 1950, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[10]  G. Kerley Equations of state for hydrogen and deuterium. , 2003 .

[11]  H B Radousky,et al.  Precision shock tuning on the national ignition facility. , 2012, Physical review letters.

[12]  R. D. Richtmyer Taylor instability in shock acceleration of compressible fluids , 1960 .

[13]  Nakai,et al.  Radiative heating of low-Z solid foils by laser-generated x rays. , 1995, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[14]  Robert L. Kauffman,et al.  Dante soft x-ray power diagnostic for National Ignition Facility , 2004 .

[15]  R J Wallace,et al.  The first measurements of soft x-ray flux from ignition scale Hohlraums at the National Ignition Facility using DANTE (invited). , 2010, The Review of scientific instruments.

[16]  J. Moody,et al.  Shock timing measurements and analysis in deuterium-tritium-ice layered capsule implosions on NIF , 2014 .

[17]  P. Souers,et al.  Hydrogen Properties for Fusion Energy , 1986 .

[18]  D. A. Callahan,et al.  Fuel gain exceeding unity in an inertially confined fusion implosion , 2014, Nature.

[19]  Measurements of the effects of the intensity pickets on laser imprinting for direct-drive, adiabat-shaping designs on OMEGA , 2007 .

[20]  R. Betti,et al.  Theory of Laser-Induced Adiabat Shaping in Inertial Fusion Implosions , 2002 .

[21]  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 .

[22]  D. Clark,et al.  The effects of early time laser drive on hydrodynamic instability growth in National Ignition Facility implosions , 2014 .

[23]  L. M. Barker,et al.  Laser interferometer for measuring high velocities of any reflecting surface , 1972 .

[24]  David K. Bradley,et al.  Line-imaging velocimeter for shock diagnostics at the OMEGA laser facility , 2004 .

[25]  O A Hurricane,et al.  Reduced instability growth with high-adiabat high-foot implosions at the National Ignition Facility. , 2014, Physical review. E, Statistical, nonlinear, and soft matter physics.

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

[27]  J. Knauer,et al.  Theory of laser-induced adiabat shaping in inertial fusion implosions: The relaxation method , 2005 .

[28]  S. Skupsky,et al.  Improved performance of direct-drive inertial confinement fusion target designs with adiabat shaping using an intensity picket , 2003 .

[29]  O. Landen,et al.  X-ray driven implosions at ignition relevant velocities on the National Ignition Facilitya) , 2013 .

[30]  V. Goncharov Theory of the Ablative Richtmyer-Meshkov Instability , 1999 .

[31]  D. Clark,et al.  Differential ablator-fuel adiabat tuning in indirect-drive implosions. , 2014, Physical review. E, Statistical, nonlinear, and soft matter physics.

[32]  L. J. Atherton,et al.  Point design targets, specifications, and requirements for the 2010 ignition campaign on the National Ignition Facility , 2010 .