Effects of drive pulse shape on graded metal pushered single shell capsule implosions on the National Ignition Facility

Author:

Dewald E. L.1ORCID,MacLaren S. A.1ORCID,Ho D. D.-M.1ORCID,Martinez D. A.1ORCID,Pino J. E.1ORCID,Tipton R. E.1,Young C. V.1ORCID,Horwood C.1ORCID,Divol L.1ORCID,Rubery M. S.1ORCID,Moore A.1ORCID,Vazsonyi A. R.1ORCID,Mellos G.1,Montgomery W.1ORCID,Smalyuk V. A.1ORCID,Graziani F.1ORCID,Monzon E.1ORCID,Prisbrey S. T.1,Whitley H. D.1ORCID,Xu H.2ORCID,Huang H.2ORCID,Kong C.2ORCID,Ratledge M.2,Volegov P.3ORCID,Freeman M. S.3ORCID,Wilde C.3ORCID,Meaney K.3ORCID

Affiliation:

1. Lawrence Livermore National Laboratory 1 , P.O. Box 808, Livermore, California 94550, USA

2. General Atomics 2 , San Diego, California 92186, USA

3. Los Alamos National Laboratory 3 , Los Alamos, New Mexico 87545, USA

Abstract

Graded metal pushered single shells (PSS) are a viable alternative to low-Z capsules (Z is the atomic number) for indirect drive inertial confinement fusion implosions due to enhanced core tamping and radiation trapping, but they can be compromised by the pusher mixing with the fuel. We compare 2-shock and 3-shock laser pulses for Be/Cr PSS capsules filled with deuterium–tritium gas fuel at 6 mg/cc density. 1D radiation-hydrodynamic simulations predict higher core compression and, hence, ∼2× higher fusion yield for the 3-shock drive than for 2-shock. Nevertheless, we observe similar core ion temperatures and fusion yields for both drives. The implosion burn duration is 25% shorter and the core volume is ∼2.5× smaller for the 3-shock drive than for 2-shock, consistent with a higher compression. 1D LASNEX mix simulations using a buoyancy-drag model matching the measured yields also agree with the observed core sizes and burn durations and suggest ∼40% and ∼70% yield degradations for 2-shock and 3-shock drives due to hydrodynamic instabilities and atomic mix at the pusher–fuel interface. At the same time, 2D HYDRA simulations show that mid-mode (2–250) instability degradations are negligible for the 2-shock implosion (9%) and significant (45%) for 3-shock. Subtracting these from the 1D mix simulations, we infer similar degradations from high-mode instabilities and atomic mix for both drives. Due to its robustness to mid-mode instabilities, future pusher–gas mix studies will use the 2-shock drive.

Funder

Lawrence Livermore National Laboratory

Publisher

AIP Publishing

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