The Physics of Long- and Intermediate-Wavelength Asymmetries of the Hot Spot
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[1] P. B. Radha,et al. Neutron yield study of direct-drive, low-adiabat cryogenic D2 implosions on OMEGA laser system , 2009 .
[2] Jianfa Gu,et al. Asymmetric-shell ignition capsule design to tune the low-mode asymmetry during the peak drive , 2016 .
[3] O. Landen,et al. The physics basis for ignition using indirect-drive targets on the National Ignition Facility , 2004 .
[4] J. Milovich,et al. Mitigating the impact of hohlraum asymmetries in National Ignition Facility implosions using capsule shims , 2016 .
[5] Peter A. Amendt,et al. Assessing the prospects for achieving double-shell ignition on the National Ignition Facility using vacuum hohlraums , 2007 .
[6] D. K. Bradley,et al. Metrics for long wavelength asymmetries in inertial confinement fusion implosions on the National Ignition Facility , 2014 .
[7] Jing-qin Su,et al. First Investigation on the Radiation Field of the Spherical Hohlraum. , 2016, Physical review letters.
[8] J. A. Marozas,et al. Theory of hydro-equivalent ignition for inertial fusion and its applications to OMEGA and the National Ignition Facilitya) , 2014 .
[9] J. A. Marozas,et al. Improving the hot-spot pressure and demonstrating ignition hydrodynamic equivalence in cryogenic deuterium–tritium implosions on OMEGAa) , 2014 .
[10] J. Lindl. Development of the indirect‐drive approach to inertial confinement fusion and the target physics basis for ignition and gain , 1995 .
[11] Karen S. Anderson,et al. Thermonuclear ignition in inertial confinement fusion and comparison with magnetic confinement , 2010 .
[12] S. Atzeni,et al. Nonlinear evolution of localized perturbations in the deceleration-phase Rayleigh-Taylor instability of an inertial confinement fusion capsule , 2007 .
[13] O A Hurricane,et al. Development of Improved Radiation Drive Environment for High Foot Implosions at the National Ignition Facility. , 2016, Physical review letters.
[14] Thomas J. Murphy,et al. The effect of turbulent kinetic energy on inferred ion temperature from neutron spectra , 2014 .
[15] V. Goncharov,et al. Performance of Direct-Drive Cryogenic Targets on OMEGA , 2007 .
[16] S. Skupsky,et al. Deceleration phase of inertial confinement fusion implosions , 2002 .
[17] Hydrodynamic scaling of the deceleration-phase Rayleigh–Taylor instability , 2013 .
[18] R. Betti,et al. Alpha Heating and Burning Plasmas in Inertial Confinement Fusion , 2015, Physical review letters.
[19] John Kelly,et al. Crossed-beam energy transfer in direct-drive implosions , 2011 .
[20] J Edwards,et al. Generalized measurable ignition criterion for inertial confinement fusion. , 2010, Physical review letters.
[21] Roy Kishony,et al. Ignition condition and gain prediction for perturbed inertial confinement fusion targets , 2001 .
[22] V N Goncharov,et al. Demonstration of Fuel Hot-Spot Pressure in Excess of 50 Gbar for Direct-Drive, Layered Deuterium-Tritium Implosions on OMEGA. , 2016, Physical review letters.
[23] J. Kilkenny,et al. Mode 1 drive asymmetry in inertial confinement fusion implosions on the National Ignition Facility , 2014 .
[24] Kelli Humbird,et al. Zonal flow generation in inertial confinement fusion implosions , 2017 .
[25] Epstein,et al. Effect of laser illumination nonuniformity on the analysis of time-resolved x-ray measurements in uv spherical transport experiments. , 1987, Physical review. A, General physics.
[26] J. Nuckolls,et al. Laser Compression of Matter to Super-High Densities: Thermonuclear (CTR) Applications , 1972, Nature.
[27] V N Goncharov,et al. Core conditions for alpha heating attained in direct-drive inertial confinement fusion. , 2016, Physical review. E.
[28] K. Mikaelian. Solution to Rayleigh-Taylor instabilities: Bubbles, spikes, and their scalings. , 2014, Physical review. E, Statistical, nonlinear, and soft matter physics.
[29] Josselin Garnier,et al. Self-consistent analysis of the hot spot dynamics for inertial confinement fusion capsules , 2005 .
[30] H. Bosch,et al. ERRATUM: Improved formulas for fusion cross-sections and thermal reactivities , 1992 .
[31] R. Betti,et al. Hot-spot dynamics and deceleration-phase Rayleigh–Taylor instability of imploding inertial confinement fusion capsules , 2001 .
[32] P. B. Radha,et al. Direct-drive inertial confinement fusion: A review , 2015 .
[33] O. Landen,et al. Integrated modeling of cryogenic layered highfoot experiments at the NIF , 2016 .
[34] R. Betti,et al. Analytical model of the ablative Rayleigh-Taylor instability in the deceleration phase , 2005 .
[35] R. Betti,et al. Inertial-confinement fusion with lasers , 2016, Nature Physics.
[36] Mark J. Schmitt,et al. Low Fuel Convergence Path to Direct-Drive Fusion Ignition. , 2016, Physical review letters.
[37] Riccardo Betti,et al. A measurable Lawson criterion and hydro-equivalent curves for inertial confinement fusion , 2008 .