EPJ Web of Conferences
Volume 59, 2013IFSA 2011 – Seventh International Conference on Inertial Fusion Sciences and Applications
|Number of page(s)||5|
|Section||III. Alternative Target Physics (Impact, Shock, Fast Ignition, ...)|
|Published online||15 November 2013|
Cone-guided fast ignition with no imposed magnetic fields
Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
a e-mail: firstname.lastname@example.org
Published online: 15 November 2013
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 1.5 MeV fast electrons, without E and B fields, ignition can be achieved with fast electron energy Efig = 30kJ. 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 = ηJb gives Efig = 20kJ, while using the full Ohm's law gives Efig > 40 kJ. This is due to magnetic self-guiding in the former case, and ∇n ×∇T magnetic fields in the latter. Using a realistic, quasi two-temperature energy spectrum derived from PIC laser-plasma simulations increases Efig to (102, 81, 162) kJ for (no E/B, E = ηJb, full Ohm's law). Such electrons are too energetic to stop in the optimal hot spot depth.
© Owned by the authors, published by EDP Sciences, 2013
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