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.

Vulcan petawatt-operation and development

Journal De Physique. IV : JP 133 (2006) 555-559

Authors:

C Hernandez-Gomez, PA Brummitt, DJ Canny, RJ Clarke, J Collier, CN Danson, AM Dunne, B Fell, AJ Frackiewicz, S Hancock, S Hawkes, R Heathcote, P Holligan, MHR Hutchinson, A Kidd, WJ Lester, IO Musgrave, D Neely, DR Neville, PA Norreys, DA Pepler, CJ Reason, W Shaikh, TB Winstone, BE Wyborn

Abstract:

Petawatt capability on the Vulcan laser facility has been available to the international plasma physics community for over two years. This has enabled novel experiments to be carried out and new regimes of physics to be explored. During that time, there have been 10 successful user experiments with 89% of shots delivered within the requested energy limits. In the autumn of 2004, pulses with powers of more than a petawatt (1015Watts) were delivered to target with energies greater than 400 J and pulse widths shorter than 500 femtoseconds (10-15) on target. In parallel to the development of ultra-high intensity pulses is a programme to enhance Vulcan's long pulse capabilities. This paper will present an overview of the current capabilities of the Vulcan Petawatt facility and discuss some of the recent technological advances that have enabled the generation of Petawatt pulses. © EDP Sciences.