Temperature measurements of shocked crystals by use of nanosecond X-ray diffraction
AIP CONF PROC 955 (2007) 325-328
Abstract:
Over the past few years we have been pioneering the use of sub-nanosecond X-ray diffraction to determine the phase and compression of shocked crystals. It is well known that the deviation of atoms from their ideal lattice sites due to thermal motion reduces the integrated intensity within diffraction peaks - the so-called Debye-Waller effect, and thus it is pertinent to investigate whether line ratios might be sufficiently sensitive to be used as a viable temperature diagnostic. Clearly the matter is not completely straight-forward, as the Debye frequency of a solid also varies under compression. In our initial investigations we have calculated the ratios of intensities of high-order reflections assuming various forms of the Gruneisen parameter, and have also compared these results with those obtained from Molecular Dynamics simulations. Given the photon energies of nanosecond X-ray pulses that can currently be produced, we comment on the experimental feasibility of the technique.Secondary shock formation in xenon-nitrogen mixtures
Physics of Plasmas 13:11 (2006)
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.Fast electron transport measurements on the vulcan PW laser facility
33rd EPS Conference on Plasma Physics 2006, EPS 2006 1 (2006) 237-240
Kinetic simulations of proton acceleration from ultra-thin foils
33rd EPS Conference on Plasma Physics 2006, EPS 2006 1 (2006) 268-271
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