Phys. Rev. E
80,
045401(R)
(2009)
[4 pages]
Effect of reentrant cone geometry on energy transport in intense laser-plasma interactions
K. L. Lancaster et al.
Show All Authors/Affiliations
Hide All Authors/Affiliations
K. L. Lancaster1, M. Sherlock1, J. S. Green1,2, C. D. Gregory3, P. Hakel4, K. U. Akli5, F. N. Beg6, S. N. Chen6, R. R. Freeman7, H. Habara8, R. Heathcote1, D. S. Hey5, K. Highbarger7, M. H. Key9, R. Kodama10,8, K. Krushelnick11, H. Nakamura10, M. Nakatsutsumi10, J. Pasley1,12, R. B. Stephens5, M. Storm13, M. Tampo10, W. Theobald13, L. Van Woerkom7, R. L. Weber7, M. S. Wei6, N. C. Woolsey12, T. Yabuuchi6, and P. A. Norreys1,2
1STFC Rutherford Appleton Laboratory, Chilton, Oxon OX11 0QX, United Kingdom 2Blackett Laboratory, Imperial College London, Prince Consort Road, London SW7 2BZ, United Kingdom 3LULI, Ecole Polytechnique, Palaiseau Cedex F91128, France 4Department of Physics, University of Nevada, Reno, Nevada 89557, USA 5General Atomics, P.O. Box 86508, San Diego, California 92186-5608, USA 6University of California–San Diego, 9500 Gilman Drive 0411, La Jolla, California 92093-0411, USA 7Department of Physics, Ohio State University, Columbus, Ohio 43210-1117, USA 8Institute of Laser Engineering, Osaka University, Suita, 565-0871 Osaka, Japan 9Lawrence Livermore National Laboratory, P.O. Box 808, Livermore, California 94550, USA 10Graduate School of Engineering, Osaka University, Suita, 565-0871 Osaka, Japan 11University of Michigan, Ann Arbour, Michigan 48109-2099, USA 12Department of Physics, University of York, Heslington, York YO10 5DD, United Kingdom 13Laboratory of Laser Energetics, University of Rochester, 250 East River Road, Rochester, New York 14623, USA
Received 3 February 2009; published 22 October 2009
The energy transport in cone-guided low-Z targets has been studied for laser intensities on target of 2.5×1020 W cm−2. Extreme ultraviolet (XUV) imaging and transverse optical shadowgraphy of the rear surfaces of slab and cone-slab targets show that the cone geometry strongly influences the observed transport patterns. The XUV intensity showed an average spot size of 65±10 μm for slab targets. The cone slabs showed a reduced spot size of 44±10 μm. The shadowgraphy for the aforementioned shots demonstrate the same behavior. The transverse size of the expansion pattern was 357±32 μm for the slabs and reduced to 210±30 μm. A transport model was constructed which showed that the change in transport pattern is due to suppression of refluxing electrons in the material surrounding the cone.
© 2009 The American Physical Society
URL:
http://link.aps.org/doi/10.1103/PhysRevE.80.045401
DOI:
10.1103/PhysRevE.80.045401
|
|