Developing one-dimensional implosions for inertial confinement fusion science. (12th December 2016)

• Record Type: Journal Article
• Authors: Kline, J. L.; Yi, S. A.; Simakov, A. N.; Olson, R. E.; Wilson, D. C.; Kyrala, G. A.; Perry, T. S.; Batha, S. H.; Dewald, E. L.; Ralph, J. E.; Strozzi, D. J.; MacPhee, A. G.; Callahan, D. A.; Hinkel, D.; Hurricane, O. A.; Leeper, R. J.; Zylstra, A. B.; Peterson, R. R.; Haines, B. M.; Yin, L.; Bradley, P. A.; Shah, R. C.; Braun, T.; Biener, J.; Kozioziemski, B. J.; Sater, J. D.; Biener, M. M.; Hamza, A. V.; Nikroo, A.; Berzak Hopkins, L. F.; Ho, D.; LePape, S.; Meezan, N. B.; Montgomery, D. S.; Daughton, W. S.; Merritt, E. C.; Cardenas, T.; Dodd, E. S.;
• Is Part Of: High power laser science and engineering. Volume 4(2016)
• Publication Date: 2016-12-12
• Subjects: beryllium capsules, -- double shells, -- inertial confinement fusion, -- liquid layers; High power lasers -- Periodicals; 621.366
• DOI: 10.1017/hpl.2016.43
• Languages: English
• ISSNs: 2095-4719

Abstract

Abstract : Experiments on the National Ignition Facility show that multi-dimensional effects currently dominate the implosion performance. Low mode implosion symmetry and hydrodynamic instabilities seeded by capsule mounting features appear to be two key limiting factors for implosion performance. One reason these factors have a large impact on the performance of inertial confinement fusion implosions is the high convergence required to achieve high fusion gains. To tackle these problems, a predictable implosion platform is needed meaning experiments must trade-off high gain for performance. LANL has adopted three main approaches to develop a one-dimensional (1D) implosion platform where 1D means measured yield over the 1D clean calculation. A high adiabat, low convergence platform is being developed using beryllium capsules enabling larger case-to-capsule ratios to improve symmetry. The second approach is liquid fuel layers using wetted foam targets. With liquid fuel layers, the implosion convergence can be controlled via the initial vapor pressure set by the target fielding temperature. The last method is double shell targets. For double shells, the smaller inner shell houses the DT fuel and the convergence of this cavity is relatively small compared to hot spot ignition. However, double shell targets have a different set of trade-off versus advantages. Details for each of these approaches are described.