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Phys. Rev. E 82, 016407 (2010) [6 pages]

Proton radiography of a shock-compressed target

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A. Ravasio1, L. Romagnani2, S. Le Pape3, A. Benuzzi-Mounaix1, C. Cecchetti2, D. Batani4, T. Boehly5, M. Borghesi2, R. Dezulian4, L. Gremillet6, E. Henry6, D. Hicks3, B. Loupias1, A. MacKinnon3, N. Ozaki1, H. S. Park3, P. Patel3, A. Schiavi7, T. Vinci1, R. Clarke8, M. Notley8, S. Bandyopadhyay8, and M. Koenig1
1Laboratoire pour l’Utilisation des Lasers Intenses, UMR 7605, CNRS–CEA–Université Paris VI–Ecole Polytechnique, 91128 Palaiseau Cedex, France
2School of Mathematics and Physics, The Queen’s University of Belfast, Belfast BT7 INN, United Kingdom
3Lawrence Livermore National Laboratory, Livermore, California 94550, USA
4Dipartimento di Fisica G. Occhialini, Universitá di Milano-Bicocca, Piazza Della Scienze 3, 20126 Milano, Italy
5Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
6CEA, DAM, DIF, F-91297 Arpajon Cedex, France
7Department of Energetics, University of Rome “La Sapienza,” Rome, Italy
8CCLRC, Rutherford Appleton Laboratory, Chilton, Didcot OX11 0QX, United Kingdom

Received 12 February 2010; published 26 July 2010

In this paper we report on the radiography of a shock-compressed target using laser produced proton beams. A low-density carbon foam target was shock compressed by long pulse high-energy laser beams. The shock front was transversally probed with a proton beam produced in the interaction of a high intensity laser beam with a gold foil. We show that from radiography data, the density profile in the shocked target can be deduced using Monte Carlo simulations. By changing the delay between long and short pulse beams, we could probe different plasma conditions and structures, demonstrating that the details of the steep density gradient can be resolved. This technique is validated as a diagnostic for the investigation of warm dense plasmas, allowing an in situ characterization of high-density contrasted plasmas.

© 2010 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevE.82.016407
DOI:
10.1103/PhysRevE.82.016407
PACS:
52.50.Lp, 52.25.Tx, 52.50.Jm