X-ray drive of beryllium capsule implosions at the National Ignition Facility

9th International Conference on Inertial Fusion Sciences and Applications

Wilson, D.C.^1 ; Yi, S.A.^1 ; Simakov, A.N.^1 ; Kline, J.L.^1 ; Kyrala, G.A.^1 ; Dewald, E.L.^2 ; Tommasini, R.^2 ; Ralph, J.E.^2 ; Olson, R.E.^1 ; Strozzi, D.J.^2 ; Celliers, P.M.^2 ; Schneider, M.B.^2 ; Macphee, A.G.^2 ; Zylstra, A.B.^1 ; Callahan, D.A.^2 ; Hurricane, O.A.^2 ; Milovich, J.L.^2 ; Hinkel, D.E.^2 ; Rygg, J.R.^2 ; Rinderknecht, H.G.^2 ; Sio, H.^3 ; Perry, T.S.^1 ; Batha, S.^1

Los Alamos National Laboratory, Los Alamos

NM, United States^1

Lawrence Livermore National Laboratory, Livermore

CA, United States^2

Massachusetts Institute of Technology, Cambridge

MA, United States^3

关键词: Hohlraums;    Laser drive;    National ignition facility;    Plastic capsule;    Shock timing;    Time dependence;    Total flux;    X-ray flux;   

Others  :  https://iopscience.iop.org/article/10.1088/1742-6596/717/1/012058/pdf
DOI  :  10.1088/1742-6596/717/1/012058

来源: IOP

【 摘 要 】

National Ignition Facility experiments with beryllium capsules have followed a path begun with "high-foot" plastic capsule implosions. Three shock timing keyhole targets, one symmetry capsule, a streaked backlit capsule, and a 2D backlit capsule were fielded before the DT layered shot. After backscatter subtraction, laser drive degradation is needed to match observed X-ray drives. VISAR measurements determined drive degradation for the picket, trough, and second pulse. Time dependence of the total Dante flux reflects degradation of the of the third laser pulse. The same drive degradation that matches Dante data for three beryllium shots matches Dante and bangtimes for plastic shots N130501 and N130812. In the picket of both Be and CH hohlraums, calculations over-estimate the x-ray flux > 1.8 keV by ∼100X, while calculating the total flux correctly. In beryllium calculations these X-rays cause an early expansion of the beryllium/fuel interface at ∼3 km/s. VISAR measurements gave only ∼0.3 km/s. The X-ray drive on the Be DT capsule was further degraded by an unplanned decrease of 9% in the total picket flux. This small change caused the fuel adiabat to rise from 1.8 to 2.3. The first NIF beryllium DT implosion achieved 29% of calculated yield, compared to CH capsules with 68% and 21%.