Hohlraum energetics scaling to 520 TW on the National Ignition Facilitya)
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P. Michel | J. Moody | R. Kirkwood | M. Rosen | D. Strozzi | O. Landen | B. MacGowan | E. Dewald | N. Meezan | J. Kilkenny | S. Burkhart | D. Kalantar | A. MacPhee | P. Miller | T. Suratwala | J. Bude | R. Tommasini | L. Atherton | D. Callahan | S. Dixit | E. Dzenitis | M. Edwards | D. Hinkel | O. Jones | R. Town | K. Widmann | S. Glenzer | L. Suter | J. Kline | G. Kyrala | A. Nikroo | C. Bennett | P. Wegner | M. Bowers | G. Erbert | M. Henesian | M. Hermann | K. Jancaitis | E. Moses | M. Nostrand | M. Shaw | C. Widmayer | B. Remington | J. Heebner | R. Olson | L. Lagin | A. Hamza | Marilyn Schneider | S. Regan | E. Williams | S. Haan | V. Smalyuk | H. Park | N. Izumi | H. Robey | D. Hicks | K. LaFortune | J. Lindl | D. Bradley | S. Glenn | A. Mackinnon | J. Ralph | H. Wilkens | W. Hsing | G. Grim | R. Berger | D. Larson | S. L. Pape | T. Ma | A. Moore | A. Pak | J. Folta | J. D. Nicola | P. D. Nicola | G. Brunton | L. Pelz | S. Batha | T. Doeppner | J. S. Ross | B. Wonterghem | I. Bass | S. Khan | R. Bennedetti | A. Condor | M. Montincelli | J. P. Patel | K. Lafortune | M. Schneider | S. Khan
[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] E. L. Lindman,et al. Theory of stimulated scattering processes in laser‐irradiated plasmas , 1975 .
[4] O. Landen,et al. The physics basis for ignition using indirect-drive targets on the National Ignition Facility , 2004 .
[5] John L. Kline,et al. Onset and saturation of backward stimulated Raman scattering of laser in trapping regime in three spatial dimensions , 2009 .
[6] E. T. Alger,et al. Cryogenic thermonuclear fuel implosions on the National Ignition Facility , 2012 .
[7] J. D. Moody,et al. Design of the National Ignition Facility static x-ray imager , 2001 .
[8] M. Rosen,et al. Proof of Principle experiments that demonstrate utility of cocktail hohlraums for indirect drive ignition , 2007 .
[9] P. Michel,et al. Stimulated Raman scatter analyses of experiments conducted at the National Ignition Facility a) , 2010 .
[10] Abbas Nikroo,et al. Developing depleted uranium and gold cocktail hohlraums for the National Ignition Facility , 2007 .
[11] D. S. Montgomery,et al. Recent Trident single hot spot experiments: Evidence for kinetic effects, and observation of Langmuir decay instability cascade , 2002 .
[12] B. Albright,et al. Different kλD regimes for nonlinear effects on Langmuir wavesa) , 2006 .
[13] L. Suter,et al. Drive characterization of indirect drive targets on the Nova laser (invited) , 1995 .
[14] Robert L. Kauffman,et al. Measurement of 0.1-3-keV x rays from laser plasmas , 1986 .
[15] J. Lindl. Development of the indirect‐drive approach to inertial confinement fusion and the target physics basis for ignition and gain , 1995 .
[16] 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.
[17] Langmuir decay instability cascade in laser-plasma experiments. , 2002, Physical review letters.
[18] L. Yin,et al. Observation of a transition from fluid to kinetic nonlinearities for langmuir waves driven by stimulated Raman backscatter. , 2005, Physical review letters.
[19] Robert Dewar,et al. Frequency Shift Due to Trapped Particles , 1972 .
[20] W. Mori,et al. Propagation and damping of nonlinear plasma wave packets. , 2009, Physical review letters.
[21] D. Colombant,et al. Increase in Rosseland mean opacity for inertial fusion hohlraum walls , 1998 .
[22] Robert L. Kauffman,et al. Dante soft x-ray power diagnostic for National Ignition Facility , 2004 .
[23] Edward I. Moses,et al. The National Ignition Facility: Laser Performance and First Experiments , 2005 .
[24] D. Strozzi,et al. Experimental evidence of predominantly transverse electron plasma waves driven by stimulated Raman scattering of picosecond laser pulses. , 2009, Physical review letters.
[25] Milo R. Dorr,et al. Effects of ion trapping on crossed-laser-beam stimulated Brillouin scattering , 2004 .
[26] P Datte,et al. Backscatter measurements for NIF ignition targets (invited). , 2010, The Review of scientific instruments.
[27] Scott C. Wilks,et al. Energy transfer between crossing laser beams , 1996 .
[28] 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.
[29] J. D. Moody,et al. Laser–plasma interactions in ignition‐scale hohlraum plasmas , 1996 .
[30] Max Tabak,et al. Progress in target physics and design for heavy ion fusion , 1999 .
[31] E Gullikson,et al. Soft x-ray images of the laser entrance hole of ignition hohlraums. , 2012, The Review of scientific instruments.
[32] James F. Drake,et al. Parametric Instabilities of Electromagnetic Waves in Plasmas , 1974 .
[33] Richard A. London,et al. Multi-beam effects on backscatter and its saturation in experiments with conditions relevant to ignitiona) , 2011 .
[34] D. Russell,et al. The reduced-description particle-in-cell model for the two plasmon decay instability , 2010 .
[35] M. J. Edwards,et al. Symmetric Inertial Confinement Fusion Implosions at Ultra-High Laser Energies , 2009, Science.
[36] D. K. Bradley,et al. Symmetry tuning via controlled crossed-beam energy transfer on the National Ignition Facilitya) , 2009 .
[37] P Bell,et al. Measuring symmetry of implosions in cryogenic Hohlraums at the NIF using gated x-ray detectors (invited). , 2010, The Review of scientific instruments.
[38] T. M. O'Neil,et al. Nonlinear Frequency Shift of an Electron Plasma Wave , 1972 .
[39] P Bell,et al. Hot electron measurements in ignition relevant Hohlraums on the National Ignition Facility. , 2010, The Review of scientific instruments.
[40] R. B. Ehrlich,et al. Assembly of high-areal-density deuterium-tritium fuel from indirectly driven cryogenic implosions. , 2012, Physical review letters.
[41] G B Zimmerman,et al. Direct measurement of energetic electrons coupling to an imploding low-adiabat inertial confinement fusion capsule. , 2012, Physical review letters.
[42] L. J. Atherton,et al. Implosion dynamics measurements at the National Ignition Facility , 2012 .
[43] Jochen Schein,et al. Demonstration of Enhanced Radiation Drive in Hohlraums Made from a Mixture of High-Z Wall Materials , 2007 .
[44] John Lindl,et al. A generalized scaling law for the ignition energy of inertial confinement fusion capsules , 2000 .
[45] Joshua E. Rothenberg,et al. Exploring the limits of the National Ignition Facility’s capsule coupling , 2000 .
[46] S. Depierreux,et al. Nonlinear modification of laser–plasma interaction processes under crossed laser beams , 1999 .
[47] W. Mori,et al. The relative importance of fluid and kinetic frequency shifts of an electron plasma wave , 2007 .
[48] O. Landen,et al. X-ray driven implosions at ignition relevant velocities on the National Ignition Facilitya) , 2013 .
[49] J. D. Moody,et al. Symmetry tuning for ignition capsules via the symcap techniquea) , 2011 .
[50] E. Williams,et al. A variational approach to parametric instabilities in inhomogeneous plasmas IV: The mixed polarization high-frequency instability , 1997 .
[51] D. F. DuBois,et al. Nonlinear saturation of stimulated Raman scattering in laser hot spots , 1999 .
[52] D. Russell,et al. A self-consistent trapping model of driven electron plasma waves and limits on stimulated Raman scatter , 2001 .
[53] D. Russell,et al. Hot-electron production and suprathermal heat flux scaling with laser intensity from the two-plasmon–decay instability , 2012 .
[54] L. J. Atherton,et al. The velocity campaign for ignition on NIFa) , 2012 .
[55] K. Bowers,et al. Trapping induced nonlinear behavior of backward stimulated Raman scattering in multi-speckled laser beamsa) , 2011 .
[56] W. Manheimer,et al. Formation of Stationary Large Amplitude Waves in Plasmas , 1971 .
[57] J. Moody,et al. Strongly driven laser-plasma coupling , 1998 .
[58] Moody,et al. Observation of energy transfer between frequency-mismatched laser beams in a large-scale plasma. , 1996, Physical review letters.
[59] Rose,et al. Saturation of stimulated Raman scattering by the excitation of strong Langmuir turbulence. , 1993, Physical review letters.
[60] P. Michel,et al. National Ignition Campaign Hohlraum energeticsa) , 2009 .
[61] L. J. Atherton,et al. Point design targets, specifications, and requirements for the 2010 ignition campaign on the National Ignition Facility , 2010 .
[62] Gilbert W. Collins,et al. First implosion experiments with cryogenic thermonuclear fuel on the National Ignition Facility , 2011 .