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Pikuz, T.; Faenov, A.*; Ishino, Masahiko; Starikov, S. V.*; Stegailov, V. V.*; Norman, G.*; Fortov, V.*; Skobelev, I.*; Tamotsu, Satoshi*; Kato, Yoshiaki*; et al.
no journal, ,
Faenov, A.*; Pikuz, T.; Skobelev, I.*; Fortov, V.*; Colgan, J.*; Abdallah, J. Jr.*; Fukuda, Yuji; Hayashi, Yukio; Pirozhkov, A. S.; Kawase, Keigo*; et al.
no journal, ,
Pikuz, S. Jr.*; Wagenaars, E.*; Culfa, O.*; Dance, R.*; Rossall, A.*; Tallents, G.*; Faenov, A.*; Kmpfer, T.*; Schulze, K.*; Uschmann, I.*; et al.
no journal, ,
Kotaki, Hideyuki; Mori, Michiaki; Hayashi, Yukio; Kando, Masaki; Daito, Izuru; Fukuda, Yuji; Pirozhkov, A. S.; Koga, J. K.; Bulanov, S. V.
no journal, ,
Kando, Masaki; Pirozhkov, A. S.; Nakamura, Tatsufumi; Esirkepov, T. Z.; Hayashi, Yukio; Pikuz, T.; Faenov, A.*; Kotaki, Hideyuki; Koga, J. K.; Bulanov, S. V.
no journal, ,
Novel schemes for generating short-pulse, coherent XUV-X-ray photons are presented. They are the relativistic flying mirror and the high order harmonics generation at the relativistic intensities. In the flying mirror scheme, two laser pulses are employed; the driver pulse excites a nonlinear plasma wave, which eventually starts to break, and the source pulse is incident on the breaking wave. Recently, we have been seeking optimum conditions for flying mirrors to generate soft X-ray photons with currently-available lasers. We also present the results of high order harmonics generation, which can be explained with a novel mechanism.
Faenov, A.*; Pikuz, T.; Ishino, Masahiko; Starikov, S. V.*; Stegailov, V. V.*; Norman, G.*; Fortov, V. E.*; Skobelev, I. Yu.*; Tamotsu, Satoshi*; Tanaka, Momoko; et al.
no journal, ,
Koga, J. K.; Bulanov, S. V.; Esirkepov, T. Z.; Pirozhkov, A. S.; Kando, Masaki; Rosanov, N. N.*
no journal, ,
Nishiuchi, Mamiko; Pirozhkov, A. S.; Ogura, Koichi; Tanimoto, Tsuyoshi*; Sakaki, Hironao; Esirkepov, T. Z.; Yogo, Akifumi; Fukuda, Yuji; Kanasaki, Masato; Sagisaka, Akito; et al.
no journal, ,
Since the first observation of the energetic ion beam from the interaction between the Ultra-high intensity short pulse and solid density target, many experimental efforts have been extensively made in all over the world in order to extend the maximum energy of ions. In the past decade, the highest ion energy recorded is 67.5 MeV for the ps laser pulse from the building size single shot operation system and 25 MeV for the compact Ti:Sapphire laser system which can deliver repetitive sub-ps laser pulses. Here in this paper we present the extension of the maximum energy of protons from the interaction between the short-pulse compact laser system and soild thin-foil target. The laser parameters are 800 nm in wavelength, 40 fs of pulse width, 8 J of energy, 10 contrast and 3
m
4
m (FWHM) of focal spot. The achieved peak intensity is increased up to 10
Wcm
, which is also well confirmed by the measured electron temperature of 16 MeV.