Secondary shock formation in xenon-nitrogen mixtures

Physics of Plasmas 13:11 (2006)

Authors:

JF Hansen, MJ Edwards, DH Froula, AD Edens, G Gregori, T Ditmire

Abstract:

The expansion of shock waves has been studied in mediums with different opacities and heat capacities, varied in systematic ways by mixing xenon with nitrogen keeping the mass density constant. An initial shock is generated through the brief (5 ns) deposition of laser energy (5 J) on the tip of a pin surrounded by the xenon-nitrogen mixture. The initial shock is spherical, radiative, with a high Mach number, and it sends a supersonic radiatively driven heat wave far ahead of itself. The heat wave rapidly slows to a transonic regime and when its Mach number drops to ∼2 with respect to the downstream plasma, the heat wave becomes of the ablative type, driving a second shock ahead of itself to satisfy mass and momentum conservation in the heat wave reference frame. The details of this sequence of events depend, among other things, on the opacity and heat capacity of the surrounding medium. Second shock formation is observed over the entire range from 100% Xe mass fraction to 100% N2. The formation radius of the second shock as a function of Xe mass fraction is consistent with an analytical estimate. © 2006 American Institute of Physics.

Direct observation of the α-ε Transition in shocked single crystal iron

Aip Conference Proceedings 845 I (2006) 240-243

Authors:

DH Kalantar, GW Collins, JD Colvin, HM Davies, JH Eggert, J Hawreliak, HE Lorenzana, MA Meyers, K Rosolankova, MS Schneider, J Sheppard, JS Stölken, JS Wark

Abstract:

In-situ x-ray diffraction was used to study the response of single crystal iron under shock conditions. Measurements of the response of [001] iron showed a uniaxial compression of the initially bcc lattice along the shock direction by up to 6% at 13 GPa. Above this pressure, the lattice responded with a further collapse of the lattice by 15-18% and a transformation to the hcp structure. The in-situ measurements are discussed and results summarized. © 2006 American Institute of Physics.

Fast electron transport measurements on the vulcan PW laser facility

33rd EPS Conference on Plasma Physics 2006, EPS 2006 1 (2006) 237-240

Authors:

PA Norreys, KL Lancaster, JS Green, CD Gregory, KU Akli, DS Hey, JR Davies, FN Beg, S Chen, D Clark, R Heathcote, RR Freeman, H Habara, K Highbarger, MH Key, R Kodama, K Krushelnick, H Nakamura, M Nakatsutsumi, N Patel, F Perez, P Simpson, R Stephens, C Stoeckl, M Storm, M Tampo, W Theobald, R Weber, MS Wei, L Van Woerkom, N Woolsey, M Zepf

Kinetic simulations of proton acceleration from ultra-thin foils

33rd EPS Conference on Plasma Physics 2006, EPS 2006 1 (2006) 268-271

Authors:

APL Robinson, P Gibbon, M Sherlock, P Norreys, D Neely

Low energy spread 100 MeV-1 GeV electron bunches from laser wakefield acceleration at loasis

23rd International Linear Accelerator Conference, LINAC 2006 - Proceedings (2006) 806-808

Authors:

CGR Geddes, E Esarey, P Michel, B Nagler, K Nakamura, GR Plateau, CB Schroeder, BA Shadwick, C Toth, J Van Tilborg, WP Leemans, SM Hooker, AJ Gonsalves, E Michel, JR Cary, D Bruhwiler

Abstract:

Experiments at the LOASIS laboratory of LBNL recently demonstrated production of 100 MeV electron beams with low energy spread and low divergence from laser wakefield acceleration. The radiation pressure of a 10 TW laser pulse guided over 10 diffraction ranges by a plasma density channel was used to drive an intense plasma wave (wakefield), producing acceleration gradients on the order of 100 GV/m in a mm-scale channel. Beam energy has now been increased from 100 to 1000 MeV by using a cm-scale guiding channel at lower density, driven by a 40 TW laser, demonstrating the anticipated scaling to higher beam energies. Particle simulations indicate that the low energy spread beams were produced from self trapped electrons through the interplay of trapping, loading, and dephasing. Other experiments and simulations are also underway to control injection of particles into the wake, and hence improve beam quality and stability further.