• High Power Laser Science and Engineering
  • Vol. 2, Issue 4, 04000e40 (2014)
[in Chinese]* and [in Chinese]
Author Affiliations
  • AWE, Aldermaston, Reading RG7 4PR, UK
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    DOI: 10.1017/hpl.2014.45 Cite this Article Set citation alerts
    [in Chinese], [in Chinese]. High energy density physics at the Atomic Weapons Establishment[J]. High Power Laser Science and Engineering, 2014, 2(4): 04000e40 Copy Citation Text show less
    AWE’s high performance computer ‘Blackthorn’.
    Fig. 1. AWE’s high performance computer ‘Blackthorn’.
    WDM and HDM are generated in planetary and solar cores as well as within nuclear weapons.
    Fig. 2. WDM and HDM are generated in planetary and solar cores as well as within nuclear weapons.
    The HELEN laser was decommissioned in 2009 after demonstrating the feasibility of carrying out relevant high energy density physics (HEDP) experiments on laser systems.
    Fig. 3. The HELEN laser was decommissioned in 2009 after demonstrating the feasibility of carrying out relevant high energy density physics (HEDP) experiments on laser systems.
    The HELEN target chamber.
    Fig. 4. The HELEN target chamber.
    HEDP experiments at AWE followed dual tracks (albeit with a very limited number of experiments in the green underground testing (UGT) line) until nuclear testing stopped. HELEN had several upgrades, but has now been replaced by the Orion facility (NYM is a 2D hydrocode used for modelling and ICF is inertial confinement fusion).
    Fig. 5. HEDP experiments at AWE followed dual tracks (albeit with a very limited number of experiments in the green underground testing (UGT) line) until nuclear testing stopped. HELEN had several upgrades, but has now been replaced by the Orion facility (NYM is a 2D hydrocode used for modelling and ICF is inertial confinement fusion).
    Orion’s long pulse amplifier chain.
    Fig. 6. Orion’s long pulse amplifier chain.
    Inside the Orion target chamber.
    Fig. 7. Inside the Orion target chamber.
    Targets range from 3D assemblies such as the hohlraum shown as a cartoon (top left) and as an actual target (top right) to flat foils (bottom right). They range in size, but the tolerances are always very tight. The image at the bottom left is a demonstration of target manufacturing capability on a miniature scale.
    Fig. 8. Targets range from 3D assemblies such as the hohlraum shown as a cartoon (top left) and as an actual target (top right) to flat foils (bottom right). They range in size, but the tolerances are always very tight. The image at the bottom left is a demonstration of target manufacturing capability on a miniature scale.
    The Orion target chamber is peppered with ports, the majority being for diagnostic access. The TIMs are shown as the large oblong devices protruding from the chamber and the target inserter is mounted vertically at the top of the chamber.
    Fig. 9. The Orion target chamber is peppered with ports, the majority being for diagnostic access. The TIMs are shown as the large oblong devices protruding from the chamber and the target inserter is mounted vertically at the top of the chamber.
    [in Chinese], [in Chinese]. High energy density physics at the Atomic Weapons Establishment[J]. High Power Laser Science and Engineering, 2014, 2(4): 04000e40
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