57th Annual Meeting of the APS Division of Plasma Physics 
Volume 60, Number 19
Monday–Friday, November 16–20, 2015;
Savannah, Georgia
Session GI3: ICF Preheat and Drive
9:30 AM–12:30 PM, 
Tuesday, November 17, 2015
Room: Oglethorpe Auditorium
Chair: Felicie Albert, Lawrence Livermore National Laboratory
Abstract ID: BAPS.2015.DPP.GI3.4
Abstract: GI3.00004 : Quantifying the Growth of Cross-Beam Energy Transfer in Polar-Direct-Drive Implosions at the Omega Laser and National Ignition Facilities
11:00 AM–11:30 AM
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 Abstract
  Abstract   
Author:
A.K. Davis
(Laboratory for Laser Energetics, U. of Rochester)
Direct-drive inertial confinement fusion requires multiple overlapping laser 
beams that can drive the cross-beam energy transfer (CBET) instability. This 
instability is of primary concern because it can reduce the laser energy 
coupling and can affect the symmetry in a polar-direct-drive (PDD) 
configuration. An experiment was designed to determine the CBET growth by 
measuring the angularly resolved mass ablation rate and ablation-front 
trajectory in a PDD configuration. Adding a thin layer of Si over a CH shell 
generates two peaks in x-ray self-emission images that are measured with a 
time-resolved pinhole imager. The inner peak is related to the position of 
the ablation front and the outer peak corresponds to the position of the 
interface of the two layers in the plasma. The emergence of the second peak 
is used to measure the time for the laser to burn through the outer layer, 
giving the average mass ablation rate of the material. The mass ablation 
rate was measured by varying the thickness of the outer silicon layer. The 
shell trajectory and mass ablation rate measured in PDD on the pole, where 
CBET has little effect, were compared with simulations to validate the 
electron thermal-transport model. Excellent agreement was obtained when 
using a 2-D nonlocal transport model, and these observables could not be 
reproduced with flux-limited models. A similar comparison was performed on 
the equator where the CBET growth is large. Without the CBET model, the 
shell velocity and mass ablation rate were significantly overestimated by 
the simulation. Adding the CBET model reduced the drive on the equator and 
reproduced the experimental results.
This material is based upon work supported by the Department of Energy 
National Nuclear Security Administration under Award Number DE-NA0001944. In 
collaboration with, D. Cao, D. T. Michel, M. Hohenberger, R. Epstein, V. N. 
Goncharov, S. X. Hu, I. V. Igumenshchev, J. A. Marozas, D. D. Meyerhofer, P. 
B. Radha, S. P. Regan, T. C. Sangster, and D. H. Froula (Laboratory for 
Laser Energetics, U. of Rochester); M. Lafon (CEA).
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2015.DPP.GI3.4