1. Cone-guided fast ignition with no imposed magnetic fields.
- Author
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Strozzi, D., Tabak, M., Larson, D., Marinak, M., Key, M., Divol, L., Kemp, A., Bellei, C., and Shay, H.
- Subjects
SIMULATION methods & models ,ELECTRONS ,ELECTRON energy states ,OHM'S law ,TEMPERATURE - Abstract
Simulations are presented of ignition-scale fast ignition targets with the integrated Zuma-Hydra PIC-hydrodynamic capability. We consider a spherical DT fuel assembly with a carbon cone, and an artificially-collimated fast electron source. We study the role of E and B fields and the fast electron energy spectrum. For mono-energetic 1.5MeV fast electrons, without E and B fields, ignition can be achieved with fast electron energy E
f ig 30 kJ. This is 3.5 the minimal deposited ignition energy of 8.7 kJ for our fuel density of 450 g/cm³. Including E and B fields with the resistive Ohm's law E = nJb gives Ef ig = 20 kJ, while using the full Ohm's law gives Ef ig > 40 kJ. This is due to magnetic self-guiding in the former case, and ∇n x ∇T magnetic fields in the latter. Using a realistic, quasi two-temperature energy spectrum derived from PIC laser-plasma simulations increases Ef ig to (102, 81, 162) kJ for (no E/B, E = nJj , full Ohm's law). f = b Such electrons are too energetic to stop in the optimal hot spot depth. [ABSTRACT FROM AUTHOR]- Published
- 2013
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