We have designed an experiment for the National Ignition Facility to measure the Hugoniot of materials such as plastic at extreme pressures. The design employs a strong spherically converging shock launched through a solid ball of material using a hohlraum radiation drive. The shock front conditions can be characterized using X-ray radiography until background from shock coalescence overtakes the backlit signal. Shock coalescence at the center is predicted to reach tens of Gbars and can be further characterized by measuring the X-ray self-emission and 2.45 MeV neutrons emitted from the shock flash region. In this simulation design work the standard plastic sphere is replaced with a deuterated polyethylene sphere, CD2, that reaches sufficien...
Capsule implosions on the National Ignition Facility (NIF) [Lindl et al., Phys. Plasmas 11, 339 (200...
A 200 μm radius hot spot at more than 2 keV temperature, 1 g/cm[superscript 3] density has been ac...
Dense plasma foci are the most efficient devices in the production of fast neutrons proceeding from ...
Spherically expanding radiative shock waves have been observed from inertially confined implosion ex...
An accurate understanding of burn dynamics in implosions of cryogenically layered deuterium and trit...
Non-burning thermonuclear fuel implosion experiments have been fielded on the National Ignition Faci...
The first inertial confinement fusion implosion experiments with equimolar deuterium-tritium thermon...
A neutron diagnostic for inertial confinement fusion (ICF) experiments was designed and fabricated t...
Exploding pusher targets, i.e. gas-filled large aspect-ratio glass or plastic shells, driven by a st...
Deuterium-filled capsule implosion experiments that employ the dynamic hohlraum are presently being ...
The width of the energy distribution of fusion-produced neutrons is often used as an indication of t...
The development of spherical Pulse Ionisation Chambers for neutron spectroscopy on DD-fusion plasmas...
A high pressure deuterium gas target has been designed to provide high-flux fast neutrons using the ...
A series of inertial confinement fusion (ICF) capsule experiments were run on the Z machine at Sandi...
Direct-drive implosion experiments on the GEKKO XII laser (9 kJ, 0.5 μm, 2 ns) with deuterium and tr...
Capsule implosions on the National Ignition Facility (NIF) [Lindl et al., Phys. Plasmas 11, 339 (200...
A 200 μm radius hot spot at more than 2 keV temperature, 1 g/cm[superscript 3] density has been ac...
Dense plasma foci are the most efficient devices in the production of fast neutrons proceeding from ...
Spherically expanding radiative shock waves have been observed from inertially confined implosion ex...
An accurate understanding of burn dynamics in implosions of cryogenically layered deuterium and trit...
Non-burning thermonuclear fuel implosion experiments have been fielded on the National Ignition Faci...
The first inertial confinement fusion implosion experiments with equimolar deuterium-tritium thermon...
A neutron diagnostic for inertial confinement fusion (ICF) experiments was designed and fabricated t...
Exploding pusher targets, i.e. gas-filled large aspect-ratio glass or plastic shells, driven by a st...
Deuterium-filled capsule implosion experiments that employ the dynamic hohlraum are presently being ...
The width of the energy distribution of fusion-produced neutrons is often used as an indication of t...
The development of spherical Pulse Ionisation Chambers for neutron spectroscopy on DD-fusion plasmas...
A high pressure deuterium gas target has been designed to provide high-flux fast neutrons using the ...
A series of inertial confinement fusion (ICF) capsule experiments were run on the Z machine at Sandi...
Direct-drive implosion experiments on the GEKKO XII laser (9 kJ, 0.5 μm, 2 ns) with deuterium and tr...
Capsule implosions on the National Ignition Facility (NIF) [Lindl et al., Phys. Plasmas 11, 339 (200...
A 200 μm radius hot spot at more than 2 keV temperature, 1 g/cm[superscript 3] density has been ac...
Dense plasma foci are the most efficient devices in the production of fast neutrons proceeding from ...