Precision Shock Tuning On The National Ignition Facility

H F Robey,P M Celliers,J L Kline,A J Mackinnon,T R Boehly,O L Landen,J H Eggert,D Hicks,S Le Pape,D R Farley,M W Bowers,K G Krauter,D H Munro,O S Jones,J L Milovich,D Clark,B K Spears,R P J Town,S W Haan,S Dixit,M B Schneider, E L Dewald, K Widmann, J D Moody, T D Döppner,H B Radousky, A Nikroo,J J Kroll, A V Hamza, J B Horner,S D Bhandarkar, E Dzenitis, E Alger, E Giraldez,C Castro,K Moreno,C Haynam, K N LaFortune, C Widmayer,M Shaw, K Jancaitis, T Parham,D M Holunga, C F Walters, B Haid, T Malsbury, D Trummer, K R Coffee,B Burr, L V Berzins, C Choate, S J Brereton,S Azevedo,H Chandrasekaran, S Glenzer, J A Caggiano,J P Knauer,J A Frenje,D T Casey,M Gatu Johnson,F H Séguin, B K Young,M J Edwards,B M Van Wonterghem, J Kilkenny,B J MacGowan, J Atherton, J D Lindl,D D Meyerhofer, E Moses

PHYSICAL REVIEW LETTERS(2012)

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摘要
Ignition implosions on the National Ignition Facility [J. D. Lindl et al., Phys. Plasmas 11, 339 (2004)] are underway with the goal of compressing deuterium-tritium fuel to a sufficiently high areal density (rho R) to sustain a self-propagating burn wave required for fusion power gain greater than unity. These implosions are driven with a very carefully tailored sequence of four shock waves that must be timed to very high precision to keep the fuel entropy and adiabat low and rho R high. The first series of precision tuning experiments on the National Ignition Facility, which use optical diagnostics to directly measure the strength and timing of all four shocks inside a hohlraum-driven, cryogenic liquid-deuterium-filled capsule interior have now been performed. The results of these experiments are presented demonstrating a significant decrease in adiabat over previously untuned implosions. The impact of the improved shock timing is confirmed in related deuterium-tritium layered capsule implosions, which show the highest fuel compression (rho R similar to 1.0 g/cm(2)) measured to date, exceeding the previous record [V. Goncharov et al., Phys. Rev. Lett. 104, 165001 (2010)] by more than a factor of 3. The experiments also clearly reveal an issue with the 4th shock velocity, which is observed to be 20% slower than predictions from numerical simulation.
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