2015
DOI: 10.1063/1.4921947
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Cryogenic tritium-hydrogen-deuterium and deuterium-tritium layer implosions with high density carbon ablators in near-vacuum hohlraums

Abstract: Articles you may be interested inNear-vacuum hohlraums for driving fusion implosions with high density carbon ablatorsa) Phys. Plasmas 22, 056318 (2015); 10.1063/1.4921151 Progress in indirect and direct-drive planar experiments on hydrodynamic instabilities at the ablation front Phys. Plasmas 21, 122702 (2014); 10.1063/1.4903331 Soft x-ray backlighting of cryogenic implosions using a narrowband crystal imaging system (invited)a) Rev. Sci. Instrum. 85, 11E501 (2014); 10.1063/1.4890215Improving the hot-spot pre… Show more

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Cited by 63 publications
(9 citation statements)
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“…10,11 An alternative approach to minimize the impact of wall motion is to shorten the laser pulses using high density carbon (HDC) ablators in conjunction with a 2-, 3-, or 4-shock laser drive. [12][13][14][15] The denser HDC (3.5 g/cm 3 compared to the 1 g/cm 3 of CH) means an equivalent ablator mass is contained in a much thinner shell through which the first shock propagates more quickly, shortening the overall length of a shock-timed laser pulse. This allows for high-performing 3shock designs that are only 6 À 7 ns in duration, which in turn enables the removal of most of the helium fill gas (down to 0.032 mg/cm 3 in the "near-vacuum" hohlraum, or NVH), reducing the drive deficits and the uncertainties associated with laser-plasma instabilities.…”
Section: Introductionmentioning
confidence: 99%
“…10,11 An alternative approach to minimize the impact of wall motion is to shorten the laser pulses using high density carbon (HDC) ablators in conjunction with a 2-, 3-, or 4-shock laser drive. [12][13][14][15] The denser HDC (3.5 g/cm 3 compared to the 1 g/cm 3 of CH) means an equivalent ablator mass is contained in a much thinner shell through which the first shock propagates more quickly, shortening the overall length of a shock-timed laser pulse. This allows for high-performing 3shock designs that are only 6 À 7 ns in duration, which in turn enables the removal of most of the helium fill gas (down to 0.032 mg/cm 3 in the "near-vacuum" hohlraum, or NVH), reducing the drive deficits and the uncertainties associated with laser-plasma instabilities.…”
Section: Introductionmentioning
confidence: 99%
“…Unfortunately, adiabat-shaped cryogenic implosions have not yet been explored further. All the recent designs explored on the NIF, being either with different capsule materials [59][60][61] or exotic forms of hohlraums [62], are rather based on low convergence implosions. An unexpected cliff in target performances seems to appear for fuel adiabat around α 2.3, with mixing at play.…”
Section: (B) Indirect-drive Physicsmentioning
confidence: 99%
“…Only in the last few years has a targeted manufacturing process been developed for lining the interior of a NIF ICF target with an ultra-low density CH foam that is uniform and robust enough to survive wetting by liquid hydrogen [9,10]. The liquid D 2 and liquid DT wetted foam layer experiments were made possible by this new target manufacturing innovation, as well as the availability of the NIF high-density carbon capsule and near-vacuum hohlraum platform [11,12]. However, preparing a foam liner on the inner surface of the capsule is quite time consuming and costly.…”
Section: Introductionmentioning
confidence: 99%