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Indirect-drive radiation uniformity in tetrahedral hohlraums

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Tetrahedral hohlraums, by which are understood spherical hohlraums with four laser entrance holes (LEH’s) placed at or near the vertices of a tetrahedron, are proposed for the National Ignition Facility (NIF) [J. Lindl, Phys. Plasmas 2, 3933 (1995)] and the upgraded OMEGA laser [T. R. Boehly et al., Rev. Sci. Instrum. 66, 508 (1995)]. All but four of the 48 NIF beams can irradiate a tetrahedral hohlraum, assuming that 72 beam ports are provided to accommodate direct drive. On OMEGA, the target chamber provides an exact tetrahedral symmetry, permitting the irradiation of tetrahedral hohlraums with all 60 beams. Hohlraum designs are optimized using a new three-dimensional view-factor program called Buttercup, which traces all beam paths through the hohlraum and calculates the radiation flux on the capsule for different values of the albedo. Good irradiation uniformity (∼2% rms) can be obtained on the capsule at all times during the implosion, even with identical beam temporal histories, in contrast to the case of cylindrical hohlraums where ‘‘beam phasing’’ is needed.
Title: Indirect-drive radiation uniformity in tetrahedral hohlraums
Description:
Tetrahedral hohlraums, by which are understood spherical hohlraums with four laser entrance holes (LEH’s) placed at or near the vertices of a tetrahedron, are proposed for the National Ignition Facility (NIF) [J.
Lindl, Phys.
Plasmas 2, 3933 (1995)] and the upgraded OMEGA laser [T.
R.
Boehly et al.
, Rev.
Sci.
Instrum.
66, 508 (1995)].
All but four of the 48 NIF beams can irradiate a tetrahedral hohlraum, assuming that 72 beam ports are provided to accommodate direct drive.
On OMEGA, the target chamber provides an exact tetrahedral symmetry, permitting the irradiation of tetrahedral hohlraums with all 60 beams.
Hohlraum designs are optimized using a new three-dimensional view-factor program called Buttercup, which traces all beam paths through the hohlraum and calculates the radiation flux on the capsule for different values of the albedo.
Good irradiation uniformity (∼2% rms) can be obtained on the capsule at all times during the implosion, even with identical beam temporal histories, in contrast to the case of cylindrical hohlraums where ‘‘beam phasing’’ is needed.

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