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Phys. Rev. Lett. 84, 899–902 (2000)

Photonuclear Physics when a Multiterawatt Laser Pulse Interacts with Solid Targets

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K. W. D. Ledingham1, I. Spencer1, T. McCanny1, R. P. Singhal1, M. I. K. Santala2, E. Clark2, I. Watts2, F. N. Beg2, M. Zepf2, K. Krushelnick2, M. Tatarakis2, A. E. Dangor2, P. A. Norreys3, R. Allott3, D. Neely3, R. J. Clark3, A. C. Machacek4, J. S. Wark4, A. J. Cresswell5, D. C. W. Sanderson5, and J. Magill6
1Department of Physics and Astronomy, University of Glasgow, Glasgow G12 8QQ, United Kingdom
2Blackett Laboratory, Imperial College, Prince Consort Road, London SW7 2BZ, United Kingdom
3Rutherford Appleton Laboratory, Chilton, Didcot, Oxon OX11 0QX, United Kingdom
4Department of Physics, University of Oxford, Clarendon Laboratory, Oxford OX1 3PU, United Kingdom
5Scottish Universities Research/Reactor Centre, East Kilbride, Glasgow G75 0QU, United Kingdom
6European Commission, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany

Received 9 March 1999; published in the issue dated 31 January 2000

See accompanying Physics Focus

When a laser pulse of intensity 1019Wcm-2 interacts with solid targets, electrons of energies of some tens of MeV are produced. In a tantalum target, the electrons generate an intense highly directional γ-ray beam that can be used to carry out photonuclear reactions. The isotopes 11C, 38K, 62,64Cu, 63Zn, 106Ag, 140Pr, and 180Ta have been produced by (γ,n) reactions using the VULCAN laser beam. In addition, laser-induced nuclear fission in 238U has been demonstrated, a process which was theoretically predicted at such laser intensities more than ten years ago. The ratio of the 11C and the 62Cu β+ activities yields shot-by-shot temperatures of the suprathermal electrons at laser intensities of 1019Wcm-2.

© 2000 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevLett.84.899
DOI:
10.1103/PhysRevLett.84.899
PACS:
52.40.Nk, 25.20.-x, 25.85.Jg, 52.60.+h