2010
DOI: 10.1088/1367-2630/12/4/043037
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High-gain shock ignition of direct-drive ICF targets for the Laser Mégajoule

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Cited by 55 publications
(45 citation statements)
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“…Nevertheless, it is worth to [97] p = -6.87 p = -6.6 notice a significant difference in kinetic energies between initial aspect ratios, especially for low implosion velocities where the kinetic energy for ignition at A = 5 is the twice of A = 3. This should have strong implication for shock ignition at low implosion velocities [38]. Power law dependences with velocity are found the same whatever the definition of the energy (threshold or minimum for ignition) but with different exponents between A.…”
Section: Kinetic Energy Thresholdsmentioning
confidence: 73%
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“…Nevertheless, it is worth to [97] p = -6.87 p = -6.6 notice a significant difference in kinetic energies between initial aspect ratios, especially for low implosion velocities where the kinetic energy for ignition at A = 5 is the twice of A = 3. This should have strong implication for shock ignition at low implosion velocities [38]. Power law dependences with velocity are found the same whatever the definition of the energy (threshold or minimum for ignition) but with different exponents between A.…”
Section: Kinetic Energy Thresholdsmentioning
confidence: 73%
“…As already shown [38,39], when the design is far from its self-ignition kinetic energy, the spike power needed for ignition becomes well above 200 TW and thus intensities on target can trigger parametric instabilities [52,53], generates hot-electrons for which the transport can become a key issue for SI [39,52,54] and laser absorption could be reduced. For marginally igniting target, below and close to the self-ignition threshold, ignitor spike powers are reduced [38] and intensities can be close to parametric instabilities thresholds [51]. Such trade-off between reduced implosion velocity and ignition requirement leads us to design new targets that could meet both requirements and offer the opportunity to achieve tunable thermonuclear moderate gain on LMJ, as predicted for noncryogenic double-shell designs [55].…”
Section: Introductionmentioning
confidence: 94%
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“…For LMJ, directly-driven self-ignition is possible [1] with indirect-drive beam geometry with zooming [5]. Moreover, Shock Ignition (SI) [6] and its application on LMJ [7] bring a new interest for direct-drive approach because it can offer high gain for non selfigniting target and allows to investigate the self-ignition threshold [8]. In this scheme, compression phase and ignition are separated.…”
Section: Introductionmentioning
confidence: 99%
“…This very promising solution was recently proposed to ignite the Fast Ignition capsule of HiPER [12,13]. We address here the possibility of using this approach for LMJ with HiPER-like targets by a 1D-and 2D-analysis [14,15], considering the LMJ beam layout. Direct-drive shock-ignition of double shell targets [16] is also adressed.…”
Section: Introductionmentioning
confidence: 99%