Higher velocity, high-foot implosions on the National Ignition Facility lasera)
Author(s) -
D. A. Callahan,
O. A. Hurricane,
D. E. Hinkel,
T. Döppner,
T. Ma,
H.-S. Park,
M. A. Barrios,
L. Berzak Hopkins,
D. T. Casey,
C. Cerjan,
E. L. Dewald,
Thomas Dittrich,
M. J. Edwards,
S. W. Haan,
A. V. Hamza,
J. L. Kline,
J. P. Knauer,
A. L. Kritcher,
O. L. Landen,
S. Le Pape,
A. G. MacPhee,
J. L. Milovich,
A. Nikroo,
A. Pak,
P. K. Patel,
J. R. Rygg,
J. E. Ralph,
J. D. Salmonson,
B. K. Spears,
P. T. Springer,
R. Tommasini,
L. R. Benedetti,
R. M. Bionta,
E. Bond,
D. K. Bradley,
J. A. Caggiano,
J. E. Field,
D. N. Fittinghoff,
J. A. Frenje,
M. Gatu Johnson,
G. P. Grim,
R. Hatarik,
F. E. Merrill,
S. R. Nagel,
N. Izumi,
S. F. Khan,
R. P. J. Town,
D. B. Sayre,
P. L. Volegov,
C. H. Wilde
Publication year - 2015
Publication title -
physics of plasmas
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.75
H-Index - 160
eISSN - 1089-7674
pISSN - 1070-664X
DOI - 10.1063/1.4921144
Subject(s) - implosion , national ignition facility , hohlraum , physics , inertial confinement fusion , plasma , ignition system , nuclear physics , opacity , neutron , yield (engineering) , atomic physics , optics , thermodynamics
By increasing the velocity in “high foot” implosions [Dittrich et al., Phys. Rev. Lett. 112, 055002 (2014); Park et al., Phys. Rev. Lett. 112, 055001 (2014); Hurricane et al., Nature 506, 343 (2014); Hurricane et al., Phys. Plasmas 21, 056314 (2014)] on the National Ignition Facility laser, we have nearly doubled the neutron yield and the hotspot pressure as compared to the implosions reported upon last year. The implosion velocity has been increased using a combination of the laser (higher power and energy), the hohlraum (depleted uranium wall material with higher opacity and lower specific heat than gold hohlraums), and the capsule (thinner capsules with less mass). We find that the neutron yield from these experiments scales systematically with a velocity-like parameter of the square root of the laser energy divided by the ablator mass. By connecting this parameter with the inferred implosion velocity ( v), we find that for shots with primary yield >1 × 1015 neutrons, the total yield ∼ v9.4. This incre...
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