Laboratory experiments on plasma jets in a magnetic field using high-power lasers

EPJ Web of Conferences 59 (2013)

Authors:

K Nishio, Y Sakawa, Y Kuramitsu, T Morita, T Ide, M Kuwada, M Koga, T Kato, T Norimatsu, C Gregory, N Woolsey, C Murphy, G Gregori, K Schaar, A Diziere, M Koenig, A Pelka, S Wang, Q Dong, Y Li, H Takabe

Abstract:

The experiments to simulate astrophysical jet generation are performed using Gekko XII (GXII) HIPER laser system at the Institute of Laser Engineering. In the experiments a fast plasma flow generated by shooting a CH plane (10 μm thickness) is observed at the rear side of the plane. By separating the focal spot of the main beams, a non-uniform plasma is generated. The non-uniform plasma flow in an external magnetic field (0.2∼0.3 T) perpendicular to the plasma is more collimated than that without the external magnetic field. The plasma β, the ratio between the plasma and magnetic pressure, is ≠1, and the magnetic Reynolds number is ∼150 in the collimated plasma. It is considered that the magnetic field is distorted by the plasma flow and enhances the jet collimation. © Owned by the authors, published by EDP Sciences, 2013.

Polarization-controlled quasi-phase matching for linearly and circularly polarized high harmonic generation

Optics InfoBase Conference Papers (2013)

Authors:

LZ Liu, K O'Keeffe, SM Hooker

The role of collisions on mode competition between the two-stream and Weibel instabilities

Journal of Plasma Physics 79:6 (2013) 987-989

Authors:

KA Humphrey, RMGM Trines, DC Speirs, P Norreys, R Bingham

Abstract:

We present results from numerical simulations conducted to investigate a potential method for realizing the required fusion fuel heating in the fast ignition scheme to achieving inertial confinement fusion. A comparison will be made between collisionless and collisional particle-in-cell simulations of the relaxation of a non-thermal electron beam through the two-stream instability. The results presented demonstrate energy transfer to the plasma ion population from the laser-driven electron beam via the nonlinear wave-wave interaction associated with the two-stream instability. Evidence will also be provided for the effects of preferential damping of competing instabilities such as the Weibel mode found to be detrimental to the ion heating process. © Cambridge University Press 2013.

A robust plasma-based laser amplifier via stimulated Brillouin scattering

(2013)

Authors:

Paulo Alves, Raoul Trines, Kathryn Humphrey, Robert Bingham, Alan Cairns, Frederico Fiuza, Ricardo Fonseca, Luis Silva, Peter Norreys

Fourier-transform inelastic X-ray scattering from time- and momentum-dependent phonon-phonon correlations

Nature Physics (2013)

Authors:

M Trigo, M Fuchs, J Chen, MP Jiang, AM Lindenberg, DA Reis, K Gaffney, S Ghimire, ME Kozina, G Ndabashimiye, M Cammarata, DM Fritz, H Lemke, D Zhu, S Fahy, A Higginbotham, JS Wark, SL Johnson, J Larsson, F Quirin, K Sokolowski-Tinten, C Uher, G Wang

Abstract:

The macroscopic characteristics of a material are determined by its elementary excitations, which dictate the response of the system to external stimuli. The spectrum of excitations is related to fluctuations in the density-density correlations and is typically measured through frequency-domain neutron or X-ray scattering. Time-domain measurements of these correlations could yield a more direct way to investigate the excitations of solids and their couplings both near to and far from equilibrium. Here we show that we can access large portions of the phonon dispersion of germanium by measuring the diffuse scattering from femtosecond X-ray free-electron laser pulses. A femtosecond optical laser pulse slightly quenches the vibrational frequencies, producing pairs of high-wavevector phonons with opposite momenta. These phonons manifest themselves as time-dependent coherences in the displacement correlations probed by the X-ray scattering. As the coherences are preferentially created in regions of strong electron-phonon coupling, the time-resolved approach is a natural spectroscopic tool for probing low-energy collective excitations in solids, and their microscopic interactions.