2006
DOI: 10.1088/0741-3335/48/12b/s07
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Target design for ignition experiments on the laser Mégajoule facility

Abstract: The adoption of a non-uniform dopant profile has substantially increased the tolerance to high mode deformations of our baseline indirect-drive design. In addition, a low deuterium-tritium (DT) gas density, obtained by 'dynamic quenching' at 2.3 K below triple point, could partly compensate for the decrease in robustness due to DT ageing. Finally, the net margin regarding all laser and target technological defects is about 2. As soon as a sufficient amount of laser beams and diagnostics is available, we will s… Show more

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Cited by 31 publications
(22 citation statements)
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“…Assuming relatively small láser beams, with surfaces of about 10 2 -15 2 cm 2 and máximum energy fluence of 1 -=-3 J/cm 2 , it turns out that a total of a few thousand beamlets should be used to provide a total energy of about 1 MJ. These beamlets should be grouped in bundles which surface would be of about 1 -1.5 m 2 (which is roughly the double of a quad in the National Ignition Facility [12] in the USA or the Láser MegaJoule [13] . Moreover, the large number of beamlets is also useful in order to use the zooming technique [14] where different focal spots are used to optimize the laser-capsule coupling preserving the irradiation uniformity of the capsule [15].…”
Section: Introductionmentioning
confidence: 99%
“…Assuming relatively small láser beams, with surfaces of about 10 2 -15 2 cm 2 and máximum energy fluence of 1 -=-3 J/cm 2 , it turns out that a total of a few thousand beamlets should be used to provide a total energy of about 1 MJ. These beamlets should be grouped in bundles which surface would be of about 1 -1.5 m 2 (which is roughly the double of a quad in the National Ignition Facility [12] in the USA or the Láser MegaJoule [13] . Moreover, the large number of beamlets is also useful in order to use the zooming technique [14] where different focal spots are used to optimize the laser-capsule coupling preserving the irradiation uniformity of the capsule [15].…”
Section: Introductionmentioning
confidence: 99%
“…Present laser facilities designed for ICF study almost all operate at blue light (3ω), such as the National Ignition Facility [2], the Shenguang series [3,4], the OAMEG [5] and the Laser Mégajoule facility [6], because 3ω has the advantages of a higher laser deposition [7,8] and a lower LPI [9] than green light (2ω). However, 3ω is generated via the frequency-tripling technique with a relatively low efficiency, and in addition, it has a relatively low damage threshold for the optic components in the final optic assembly [10].…”
Section: Introductionmentioning
confidence: 99%
“…Two laser facilities are built to achieve ICF with indirect drive configuration: the National Ignition Facility (NIF) in U.S.A. [3] and the Laser MégaJoule (LMJ) in France [4]. For LMJ, directly-driven self-ignition is possible [1] with indirect-drive beam geometry with zooming [5].…”
Section: Introductionmentioning
confidence: 99%
“…In this scheme, compression phase and ignition are separated. Usually, targets designs present high initial aspect ratio A, defined as the ratio of the deuterium-tritium (DT) ice-layer inner radius over the DT-ice layer thickness, around A = 7 for Fast-Ignition (FI) [9] or for Direct-Drive (DD) targets [1] and around A = 11 for indirect drive targets [4]. In our study, we explore low initial aspect ratios and moderate implosion velocities.…”
Section: Introductionmentioning
confidence: 99%