First implosion experiments with cryogenic thermonuclear fuel on the National Ignition Facility
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Gilbert W. Collins | P. Michel | L. Divol | J. Moody | R. Kirkwood | O. Landen | B. MacGowan | B. V. Wonterghem | J. Ross | E. Dewald | N. Meezan | D. Clark | J. Kilkenny | D. Kalantar | A. MacPhee | L. Atherton | D. Callahan | S. Dixit | E. Dzenitis | C. Haynam | O. Jones | J. Milovich | C. Thomas | R. Town | S. Weber | K. Widmann | S. Glenzer | L. Suter | J. Kline | G. Kyrala | A. Nikroo | J. Knauer | R. Petrasso | F. Séguin | M. Shoup | T. Parham | P. Wegner | G. Heestand | E. Moses | C. Orth | M. Shaw | C. Widmayer | P. Whitman | C. Cerjan | R. Olson | Marilyn Schneider | B. Spears | P. McKenty | S. Regan | D. Munro | S. Haan | V. Glebov | E. Giraldez | N. Izumi | P. Patel | H. Robey | D. Casey | S. Hatchett | R. Leeper | D. Hicks | K. LaFortune | J. Lindl | D. Bradley | S. Glenn | A. Mackinnon | P. Springer | B. Hammel | J. Salmonson | K. Moreno | J. Ralph | J. Kroll | J. Horner | E. Alger | R. Berger | D. Bleuel | J. Caggiano | C. Castro | C. Choate | T. Döppner | R. Dylla‐Spears | J. Fair | L. Frenje | M. G. Johnson | H. Huang | A. Kritcher | D. Larson | S. L. Pape | T. Ma | E. Mapoles | A. Moore | M. Moran | B. Nathan | A. Pak | H. Rinderknecht | J. Sater | C. Sangster | W. Stoeffl | C. Walters | M. Edwards | J. D. Nicola | P. D. Nicola | B. Kozioziemski | R. Heeter | H. Herrmann | D. Holunga | Douglas Wilson | B. Wonterghem | H. Huang | K. Lafortune | J. Kroll | M. Schneider
[1] J D Lindl,et al. Tuning the implosion symmetry of ICF targets via controlled crossed-beam energy transfer. , 2009, Physical review letters.
[2] Peter M. Celliers,et al. Capsule implosion optimization during the indirect-drive National Ignition Campaign , 2010 .
[3] Kunioki Mima,et al. Random Phasing of High-Power Lasers for Uniform Target Acceleration and Plasma-Instability Suppression , 1984 .
[4] O. Landen,et al. The physics basis for ignition using indirect-drive targets on the National Ignition Facility , 2004 .
[5] Otto L. Landen,et al. Status of our understanding and modeling of x-ray coupling efficiency in laser heated hohlraums , 2001 .
[6] P. B. Radha,et al. Progress in hydrodynamics theory and experiments for direct-drive and fast ignition inertial confinement fusion , 2006 .
[7] Gilbert W. Collins,et al. Velocity and timing of multiple spherically converging shock waves in liquid deuterium. , 2011, Physical review letters.
[8] Steven W. Haan,et al. Three-dimensional HYDRA simulations of National Ignition Facility targets , 2001 .
[9] Edward I. Moses,et al. Experiments and multiscale simulations of|[nbsp]|laser propagation through ignition-scale|[nbsp]|plasmas , 2007 .
[10] B. MacGowan,et al. MEASUREMENTS OF SUPRATHERMAL ELECTRONS IN HOHLRAUM PLASMAS WITH X-RAY SPECTROSCOPY , 1998 .
[11] P. B. Radha,et al. Demonstration of the highest deuterium-tritium areal density using multiple-picket cryogenic designs on OMEGA. , 2010, Physical review letters.
[12] Jay D. Salmonson,et al. Prediction of ignition implosion performance using measurements of Low-deuterium surrogates , 2010 .
[13] Jochen Schein,et al. First laser–plasma interaction and hohlraum experiments on the National Ignition Facility , 2005 .
[14] R. Betti,et al. Publisher’s Note: “A measurable Lawson criterion and hydro-equivalent curves for inertial confinement fusion” [Phys. Plasmas 15, 102707 (2008)] , 2009 .
[15] J. D. Kilkenny,et al. Diagnostic systems for the National Ignition Facility (NIF) (invited) , 1995 .
[16] J. Lindl. Development of the indirect‐drive approach to inertial confinement fusion and the target physics basis for ignition and gain , 1995 .
[17] M. J. Pivovaroff,et al. Images of the laser entrance hole from the static x-ray imager at NIF. , 2010, The Review of scientific instruments.
[18] Karen S. Anderson,et al. Thermonuclear ignition in inertial confinement fusion and comparison with magnetic confinement , 2010 .
[19] 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 .
[20] V. A. Smalyuk,et al. Diagnosing and controlling mix in National Ignition Facility implosion experiments a) , 2011 .
[21] Ramon Joe Leeper,et al. Probing high areal-density cryogenic deuterium-tritium implosions using downscattered neutron spectra measured by the magnetic recoil spectrometera) , 2010 .
[22] Edward I. Moses. The National Ignition Facility and the Promise of Inertial Fusion Energy , 2010 .
[23] Marilyn Schneider,et al. Analysis of the National Ignition Facility ignition hohlraum energetics experiments a) , 2011 .
[24] Peter A. Amendt,et al. A simple time-dependent analytic model of the P2 asymmetry in cylindrical hohlraums , 1999 .
[25] R. M. Franks,et al. Demonstration of ignition radiation temperatures in indirect-drive inertial confinement fusion hohlraums. , 2010, Physical review letters.
[26] P. Michel,et al. Energy transfer between laser beams crossing in ignition hohlraums , 2009 .
[27] Murakami,et al. Experimental observation of laser-induced radiation heat waves. , 1990, Physical review letters.
[28] David Strozzi,et al. Suprathermal electrons generated by the two-plasmon-decay instability in gas-filled Hohlraums , 2008 .
[29] P. B. Radha,et al. High-areal-density fuel assembly in direct-drive cryogenic implosions. , 2008, Physical review letters.
[30] J. Meyer-ter-Vehn,et al. The physics of inertial fusion - Hydrodynamics, dense plasma physics, beam-plasma interaction , 2004 .
[31] Hong,et al. Higher Fusion Power Gain with Current and Pressure Profile Control in Strongly Shaped DIII-D Tokamak Plasmas. , 1996, Physical review letters.
[32] J. Lawson. SOME CRITERIA FOR A POWER PRODUCING THERMONUCLEAR REACTOR , 1957 .
[33] J Edwards,et al. Generalized measurable ignition criterion for inertial confinement fusion. , 2010, Physical review letters.
[34] Robert L. Kauffman,et al. Dante soft x-ray power diagnostic for National Ignition Facility , 2004 .
[35] Edward I. Moses,et al. The National Ignition Facility: Laser Performance and First Experiments , 2005 .
[36] P Datte,et al. Backscatter measurements for NIF ignition targets (invited). , 2010, The Review of scientific instruments.
[37] Turner,et al. Modeling and interpretation of Nova's symmetry scaling data base. , 1994, Physical review letters.
[38] J. D. Moody,et al. Laser–plasma interactions in ignition‐scale hohlraum plasmas , 1996 .
[39] Peter A. Amendt,et al. Design and modeling of ignition targets for the National Ignition Facility , 1995 .
[40] L. Perkins,et al. Higher fusion power gain with profile control in DIII-D tokamak plasmas , 1997 .
[41] L. Divol,et al. Backscatter reduction using combined spatial, temporal, and polarization beam smoothing in a long-scale-length laser plasma. , 2001, Physical review letters.
[42] M. J. Edwards,et al. Symmetric Inertial Confinement Fusion Implosions at Ultra-High Laser Energies , 2009, Science.
[43] D. K. Bradley,et al. Symmetry tuning via controlled crossed-beam energy transfer on the National Ignition Facilitya) , 2009 .
[44] C. Sorce,et al. Experimental demonstration of early time, hohlraum radiation symmetry tuning for indirect drive ignition experiments , 2011 .
[45] Sergei O. Kucheyev,et al. Condensed hydrogen for thermonuclear fusion , 2010 .
[46] Daniel N. Baker,et al. The role of symmetry in indirect‐drive laser fusion , 1995 .
[47] L. Coldren,et al. Radical beam/ion beam etching of GaAs , 1988 .
[48] J. F. Briesmeister. MCNP-A General Monte Carlo N-Particle Transport Code , 1993 .
[49] Blain,et al. Energetics of Inertial Confinement Fusion Hohlraum Plasmas , 1998 .
[50] Joshua E. Rothenberg,et al. Reduction of laser self-focusing in plasma by polarization smoothing , 1998 .
[51] S. Sutton,et al. National Ignition Facility laser performance status. , 2007, Applied optics.
[52] M Keilhacker. Fusion physics progress on the Joint European Torus (JET) , 1999 .
[53] J. D. Moody,et al. Symmetry tuning for ignition capsules via the symcap techniquea) , 2011 .
[54] J. M. Mack,et al. Diagnosing inertial confinement fusion gamma ray physics (invited). , 2010, The Review of scientific instruments.
[55] Donald W. Phillion,et al. Efficient Raman sidescatter and hot-electron production in laser-plasma interaction experiments , 1984 .
[56] J D Lindl,et al. Three-wavelength scheme to optimize hohlraum coupling on the National Ignition Facility. , 2010, Physical review. E, Statistical, nonlinear, and soft matter physics.
[57] Robert Fedosejevs,et al. Stimulated Raman backscatter from a magnetically confined plasma column , 1982 .
[58] A. B. Langdon,et al. On the dominant and subdominant behavior of stimulated Raman and Brillouin scattering driven by nonuniform laser beams , 1998 .
[59] Jay D. Salmonson,et al. Robustness studies of ignition targets for the National Ignition Facility in two dimensions , 2007 .
[60] R. E. Marshak,et al. Effect of Radiation on Shock Wave Behavior , 1958 .
[61] Peter A. Amendt,et al. Demonstration of time-dependent symmetry control in hohlraums by drive-beam staggering , 2000 .
[62] R J Wallace,et al. Observation of high soft x-ray drive in large-scale hohlraums at the National Ignition Facility. , 2010, Physical review letters.
[63] Hiroshi Azechi,et al. High-density compression experiments at ILE, Osaka , 1991 .
[64] Riccardo Betti,et al. A measurable Lawson criterion and hydro-equivalent curves for inertial confinement fusion , 2008 .
[65] W. Kerner,et al. High fusion performance from deuterium-tritium plasmas in JET , 1999 .
[66] P. Michel,et al. National Ignition Campaign Hohlraum energeticsa) , 2009 .
[67] L. J. Atherton,et al. Point design targets, specifications, and requirements for the 2010 ignition campaign on the National Ignition Facility , 2010 .
[68] J. Hoffer,et al. Radioactively induced sublimation in solid tritium. , 1988, Physical review letters.