Implosion Hydrodynamics of Fast Ignition Targets

The fast ignition (FI) concept requires the generation of a compact, dense, pure fuel mass accessible to an external ignition source. The current base line FI target is a shell fitted with a reentrant cone extending to near its center. Conventional direct- or indirect-drive collapses the shell near the tip of the cone and then an ultraintense laser pulse focused to the inside cone tip generates high-energy electrons to ignite the dense fuel. A theoretical and experimental investigation was undertaken of the collapse of such targets, validating modeling, and exploring the trade-offs available, in such an asymmetric geometry, to optimize compaction of the fuel and maintain the integrity of the cone. The collapse is complex. Away from the cone, the shell collapses much as does a conventional implosion, generating a hot, low-density inner core. But because of the open side, hot plasma exhausts out toward the tip of the cone. This hot plasma is advantageous for implosion diagnostics; it can provide protons for...

[1]  H. Shiraga,et al.  Nuclear fusion: Fast heating scalable to laser fusion ignition , 2002, Nature.

[2]  Kenneth Glenn Tirsell,et al.  Absolute detection efficiency of a microchannel plate detector to x rays in the 1-100 KeV energy range , 1993, Optics & Photonics.

[3]  Gregory A. Moses,et al.  Inertial confinement fusion , 1982 .

[4]  R. Stephens,et al.  Implosion of indirectly driven reentrant-cone shell target. , 2003, Physical review letters.

[5]  Niels Bohr,et al.  INERTIAL CONFINEMENT FUSION , 2006 .

[6]  O L Landen,et al.  Hohlraum-driven high-convergence implosion experiments with multiple beam cones on the omega laser facility. , 2002, Physical review letters.

[7]  M. Rosen The physics issues that determine inertial confinement fusion target gain and driver requirements: A tutorial , 1999 .

[8]  Michael D. Perry,et al.  Ignition and high gain with ultrapowerful lasers , 1994 .

[9]  Stefano Atzeni,et al.  Inertial fusion fast ignitor: Igniting pulse parameter window vs the penetration depth of the heating particles and the density of the precompressed fuel , 1999 .

[10]  L. M. Elasky,et al.  Direct-drive cryogenic target implosion performance on OMEGA , 2003 .

[11]  N. G. Basov,et al.  Thermonuclear gain of ICF targets with direct heating of ignitor , 1992 .

[12]  N. Miyanaga,et al.  Fast heating of ultrahigh-density plasma as a step towards laser fusion ignition , 2001, Nature.

[13]  Samuel A. Letzring,et al.  Initial performance results of the OMEGA laser system , 1997 .