A high-resolution integrated model of the National Ignition Campaign cryogenic layered experimentsa)
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L. J. Atherton | J. D. Moody | C. J. Cerjan | J. D. Kilkenny | D. K. Bradley | John L. Kline | Paul T. Springer | K. N. LaFortune | John Lindl | Rebecca Dylla-Spears | C. C. Widmayer | M. J. Edwards | D. A. Callahan | Jose Milovich | Steven W. Haan | O. S. Jones | Michael M. Marinak | S. M. Sepke | Otto L. Landen | Johan A. Frenje | T. Döppner | Brian J. MacGowan | C. A. Haynam | T. R. Boehly | J. P. Knauer | Klaus Widmann | Hans W. Herrmann | Peter M. Celliers | H. F. Robey | B. K. Spears | Stephen V. Weber | D. S. Clark | Damien G. Hicks | Pierre Michel | D. H. Munro | Vladimir Yu. Glebov | D. R. Farley | G. A. Kyrala | Nathan Meezan | B. J. Haid | J. D. Sater | E. J. Bond | B. J. Kozioziemski | R. E. Olson | Laura Robin Benedetti | Ed Williams | R. P. J. Town | J. A. Caggiano | Siegfried Glenzer | James McNaney | T. G. Parham | M. J. Moran | H. L. Wilkens | Evan R. Mapoles | A. Nikroo | P. Michel | J. Moody | O. Landen | B. MacGowan | N. Meezan | D. Clark | J. Kilkenny | L. Atherton | E. Bond | D. Callahan | C. Haynam | O. Jones | J. Milovich | R. Town | S. Weber | K. Widmann | S. Glenzer | L. Suter | J. Kline | G. Kyrala | A. Nikroo | J. Knauer | J. Frenje | M. Marinak | T. Parham | C. Widmayer | C. Cerjan | R. Olson | B. Spears | S. Sepke | T. Boehly | E. Williams | D. Munro | S. Haan | V. Glebov | H. Robey | D. Wilson | P. Celliers | D. Hicks | J. Lindl | D. Bradley | S. Glenn | A. Mackinnon | P. Springer | H. Wilkens | D. Bleuel | J. Caggiano | T. Döppner | R. Dylla‐Spears | D. Farley | B. Haid | J. Mcnaney | E. Mapoles | M. Moran | J. Sater | M. Edwards | L. Benedetti | S. Dixit | M. Patel | B. Kozioziemski | H. Herrmann | M. Patel | L. J. Suter | A. J. Mackinnon | D. C. Wilson | S. M. Glenn | E. G. Dzentitis | D. L. Bleuel | S. M. Dixit | K. Lafortune
[1] D. K. Bradley,et al. Symmetry tuning via controlled crossed-beam energy transfer on the National Ignition Facilitya) , 2009 .
[2] Steven W. Haan,et al. Three-dimensional HYDRA simulations of National Ignition Facility targets , 2001 .
[3] P. Michel,et al. The role of a detailed configuration accounting (DCA) atomic physics package in explaining the energy balance in ignition-scale hohlraums , 2011 .
[4] J. M. Koning,et al. Short-wavelength and three-dimensional instability evolution in National Ignition Facility ignition capsule designs , 2011 .
[5] Jay D. Salmonson,et al. High-mode Rayleigh-Taylor growth in NIF ignition capsules , 2007 .
[6] Gregory A. Moses,et al. Inertial confinement fusion , 1982 .
[7] 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 .
[8] Peter M. Celliers,et al. Capsule implosion optimization during the indirect-drive National Ignition Campaign , 2010 .
[9] J. M. Mack,et al. Diagnosing inertial confinement fusion gamma ray physics (invited). , 2010, The Review of scientific instruments.
[10] O. L. Landen,et al. Experimental validation of a diagnostic technique for tuning the fourth shock timing on National Ignition Facility , 2010 .
[11] John Lindl,et al. A generalized scaling law for the ignition energy of inertial confinement fusion capsules , 2000 .
[12] Marilyn Schneider,et al. Analysis of the National Ignition Facility ignition hohlraum energetics experiments a) , 2011 .
[13] Robert L. Kauffman,et al. Measurement of 0.1-3-keV x rays from laser plasmas , 1986 .
[14] Gilbert W. Collins,et al. Convergent ablator performance measurements , 2010 .
[15] L. J. Atherton,et al. Point design targets, specifications, and requirements for the 2010 ignition campaign on the National Ignition Facility , 2010 .