High harmonic generation in the relativistic limit

Nature Physics 2:7 (2006) 456-459

Authors:

B Dromey, M Zepf, A Gopal, K Lancaster, MS Wei, K Krushelnick, M Tatarakis, N Vakakis, S Moustaizis, R Kodama, M Tampo, C Stoeckl, R Clarke, H Habara, D Neely, S Karsch, P Norreys

Shock Induced α‐ε Phase Change in Iron: Analysis of MD Simulations and Experiment

AIP Conference Proceedings AIP Publishing 845:1 (2006) 220-223

Authors:

J Hawreliak, K Rosolankova, JF Belak, G Collins, J Colvin, HM Davies, JH Eggert, TC Germann, B Holian, DH Kalantar, K Kadau, P Lomdahl, HE Lorenzana, J Sheppard, JS Stölken, JS Wark

Clark et al. Reply

Physical Review Letters 96:24 (2006)

Authors:

EL Clark, K Krushelnick, M Zepf, M Tatarakis, FN Beg, PA Norreys, AE Dangor

Analysis of four-wave mixing of high-power lasers for the detection of elastic photon-photon scattering

(2006)

Authors:

J Lundin, M Marklund, E Lundstrom, G Brodin, J Collier, R Bingham, JT Mendonca, P Norreys

High energy electron transport in solids

Journal De Physique. IV : JP 133 (2006) 355-360

Authors:

RB Stephens, RPJ Snavely, Y Aglitskii, KU Akli, F Amiranoff, C Andersen, D Batani, SD Baton, T Cowan, RR Freeman, JS Green, H Habara, T Hall, SP Hatchett, DS Hey, JM Hill, JL Kaae, MH Key, JA King, JA Koch, R Kodama, M Koenig, K Krushelnick, KL Lancaster, AJ MacKinnon, E Martinolli, CD Murphy, M Nakatsutsumi, P Norreys, E Perelli-Cippo, MR Le Gloahec, B Remington, C Rousseaux, JJ Santos, F Scianitti, C Stoeckl, M Tabak, KA Tanaka, W Theobald, R Town, T Yabuuchi, B Zhang

Abstract:

With the addition of recent PW shots, the propagation of short-pulse laser generated electron beams have been studied using laser pulse energies from 30 J to 300 J, generating currents up to ∼15 MA in solid Al:Cu targets. This is ∼5% of the current that will be required in an ignition pulse. To this level, the current appears to simply scale with laser power, the propagation spread not change at all. The resistance of the aluminum does not seem to play a role in the propagation characteristics, though it might in setting the current starting parameters. We do find that at the highest currents parts of these targets reach temperatures high enough to modify the Cu-K2 emission spectrum rendering our Bragg imaging mirrors ineffective; spectrometers will be needed to collect data at these higher temperatures. © EDP Sciences.