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Investigation of fast-electron-induced Kα x rays in laser-produced blow-off plasma.
Sawada, H; Wei, M S; Chawla, S; Morace, A; Akli, K; Yabuuchi, T; Nakanii, N; Key, M H; Patel, P K; Mackinnon, A J; McLean, H S; Stephens, R B; Beg, F N.
Afiliação
  • Sawada H; Center for Energy Research, University of California San Diego, La Jolla, California 92093, USA.
  • Wei MS; General Atomics, San Diego, California 92093, USA.
  • Chawla S; Center for Energy Research, University of California San Diego, La Jolla, California 92093, USA and Lawrence Livermore National Laboratory, Livermore, California 94550, USA.
  • Morace A; Center for Energy Research, University of California San Diego, La Jolla, California 92093, USA.
  • Akli K; Department of Physics, Ohio State University, Columbus, Ohio 43210, USA.
  • Yabuuchi T; Graduate School of Engineering, Osaka University, 565-0871, Japan.
  • Nakanii N; Photon Pioneers Center, Osaka University, 565-0871, Japan.
  • Key MH; Lawrence Livermore National Laboratory, Livermore, California 94550, USA.
  • Patel PK; Lawrence Livermore National Laboratory, Livermore, California 94550, USA.
  • Mackinnon AJ; Lawrence Livermore National Laboratory, Livermore, California 94550, USA.
  • McLean HS; Lawrence Livermore National Laboratory, Livermore, California 94550, USA.
  • Stephens RB; General Atomics, San Diego, California 92093, USA.
  • Beg FN; Center for Energy Research, University of California San Diego, La Jolla, California 92093, USA.
Article em En | MEDLINE | ID: mdl-24730954
ABSTRACT
Refluxing of fast electrons generated by high-intensity, short-pulse lasers was investigated by measuring electron-induced Kα x rays from a buried tracer layer. Using planar foils of Au/Cu/CH, the 150-J, 0.7-ps TITAN short-pulse laser was focused on the gold foil to generate fast electrons and the 3-ns, 300-J long pulse beam irradiated on the CH side to create expanding plasma as a conducting medium. By delaying the short-pulse beam timing from the long pulse laser irradiation, the plasma size was varied to change electron refluxing in the target rear. The total yields and two-dimensional images of 8.05-keV Cu-Kα x ray were recorded with an x-ray spectrometer and two monochromatic crystal imagers. The measurements show that the integrated yields decrease by a factor of 10 from refluxing to the nonrefluxing limit. Similar radial profiles of the Kα images in the rear were observed at all delays. Hybrid-particle-in-cell simulations using plasma profiles calculated by a radiation-hydrodynamic code HYDRA agree well with the measured Kα yields. The simulations suggest that conducting plasma with the size of ∼300 µm in the laser direction and ∼600 µm in the lateral direction at the density of 2 × 1020 1/cm3 is sufficiently large to prevent electrons from refluxing in the target. The parameters found in this study can be useful in designing experiments utilizing a Kα x-ray source in refluxing regime or a tracer layer in nonrefluxing regime.
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Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: Phys Rev E Stat Nonlin Soft Matter Phys Ano de publicação: 2014 Tipo de documento: Article
Buscar no Google
Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: Phys Rev E Stat Nonlin Soft Matter Phys Ano de publicação: 2014 Tipo de documento: Article