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Autor:
T. El Ajjouri, Fabrice Marteau, L. Chapuis, Geetanjali Sharma, D. Dennetière, Cédric Thaury, Mathieu Valléau, M. Tilmont, Marie-Agnès Tordeux, Muriel Thomasset, Nicolas Hubert, Catalin Miron, Marie Labat, Victor Malka, Yannick Dietrich, M H N’guyen, Alexandre Loulergue, Fabien Briquez, Igor Andriyash, Martin Khojoyan, Christian Herbeaux, M. E. Couprie, A Rouqier, C. Szwaj, M Vanderbergue, N. Leclercq, Alain Lestrade, François Polack, Charles Bourassin-Bouchet, W. Yang, L. Cassinari, Keihan Tavakoli, F. Bouvet, J.-L. Marlats, C. Benabderrahmane, M. El Ajjouri, Jean-Pierre Duval, Olivier Marcouillé, Guillaume Lambert, J. Vétéran, Serge Bielawski, C. Evain, D. Zerbib, P. Berteaud, Patrick Rommeluère, M Sebdouai, Xavier Davoine
Publikováno v:
'Plasma Physics and Controlled Fusion ', vol: 58, pages: 034020-1-034020-11 (2016)
Plasma Physics and Controlled Fusion
Plasma Physics and Controlled Fusion, IOP Publishing, 2016, 58 (3), ⟨10.1088/0741-3335/58/3/034020⟩
Plasma Physics and Controlled Fusion, 2016, 58 (3), ⟨10.1088/0741-3335/58/3/034020⟩
Plasma Physics and Controlled Fusion
Plasma Physics and Controlled Fusion, IOP Publishing, 2016, 58 (3), ⟨10.1088/0741-3335/58/3/034020⟩
Plasma Physics and Controlled Fusion, 2016, 58 (3), ⟨10.1088/0741-3335/58/3/034020⟩
The laser–plasma accelerator (LPA) presently provides electron beams with a typical current of a few kA, a bunch length of a few fs, energy in the few hundred MeV to several GeV range, a divergence of typically 1 mrad, an energy spread of the order