Implosion dynamics measurements at the National Ignition Facility
Authors: Hicks D. G. , Meezan N. B. , Dewald E. L. , Mackinnon A. J. , Olson R. E. , Callahan D. A. , Döppner T. , Benedetti L. R. , Bradley D. K. , Celliers P. M. , Clark D. S. , Di Nicola P. , Dixit S. N. , Dzenitis E. G. , Eggert J. E. , Farley D. R. , Frenje J. A. , Glenn S. M. , Glenzer S. H. , Hamza A. V. , Heeter R. F. , Holder J. P. , Izumi N. , Kalantar D. H. , Khan S. F. , Kline J. L. , Kroll J. J. , Kyrala G. A. , Ma T. , MacPhee A. G. , McNaney J. M. , Moody J. D. , Moran M. J. , Nathan B. R. , Nikroo A. , Opachich Y. P. , Petrasso R. D. , Prasad R. R. , Ralph J. E. , Robey H. F. , Rinderknecht H. G. , Rygg J. R. , Salmonson J. D. , Schneider M. B. , Simanovskaia N. , Spears B. K. , Tommasini R. , Widmann K. , Zylstra A. B. , Collins G. W. , Landen O. L. , Kilkenny J. D. , Hsing W. W. , MacGowan B. J. , Atherton L. J. , Edwards M. J. 
Published: December 2012

Measurements have been made of the in-flight dynamics of imploding capsules indirectly driven by laser energies of 1–1.7 MJ at the National Ignition Facility [Miller et al., Nucl. Fusion 44, 228 (2004)]. These experiments were part of the National Ignition Campaign [Landen et al., Phys. Plasmas 18, 051002 (2011)] to iteratively optimize the inputs required to achieve thermonuclear ignition in the laboratory. Using gated or streaked hard x-ray radiography, a suite of ablator performance parameters, including the time-resolved radius, velocity, mass, and thickness, have been determined throughout the acceleration history of surrogate gas-filled implosions. These measurements have been used to establish a dynamically consistent model of the ablative drive history and shell compressibility throughout the implosion trajectory. First results showed that the peak velocity of the original 1.3-MJ Ge-doped polymer (CH) point design using Au hohlraums reached only 75% of the required ignition velocity. Several capsule, hohlraum, and laser pulse changes were then implemented to improve this and other aspects of implosion performance and a dedicated effort was undertaken to test the sensitivity of the ablative drive to the rise time and length of the main laser pulse. Changing to Si rather than Ge-doped inner ablator layers and increasing the pulse length together raised peak velocity to 93% ± 5% of the ignition goal using a 1.5 MJ, 420 TW pulse. Further lengthening the pulse so that the laser remained on until the capsule reached 30% (rather than 60%–70%) of its initial radius, reduced the shell thickness and improved the final fuel ρR on companion shots with a cryogenic hydrogen fuel layer. Improved drive efficiency was observed using U rather than Au hohlraums, which was expected, and by slowing the rise time of laser pulse, which was not. The effect of changing the Si-dopant concentration and distribution, as well as the effect of using a larger initial shell thickness were also examined, both of which indicated that instabilities seeded at the ablation front are a significant source of hydrodynamic mix into the central hot spot. Additionally, a direct test of the surrogacy of cryogenic fuel layered versus gas-filled targets was performed. Together all these measurements have established the fundamental ablative-rocket relationship describing the dependence of implosion velocity on fractional ablator mass remaining. This curve shows a lower-than-expected ablator mass at a given velocity, making the capsule more susceptible to feedthrough of instabilities from the ablation front into the fuel and hot spot. This combination of low velocity and low ablator mass indicates that reaching ignition on the NIF will require &gt;20 μm (∼10%) thicker targets and laser powers at or beyond facility limits.