Transport of high-energy charged particles through spatially-intermittent turbulent magnetic fields

Astrophysical Journal American Astronomical Society 892:2 (2020) 114

Authors:

LE Chen, AFA Bott, Petros Tzeferacos, Alexandra Rigby, Anthony Bell, Robert Bingham, C Graziani, Jonathan Katz, Richard Petrasso, Gianluca Gregori, Francesco Miniati

Abstract:

Identifying the sources of the highest energy cosmic rays requires understanding how they are deflected by the stochastic, spatially intermittent intergalactic magnetic field. Here we report measurements of energetic charged-particle propagation through a laser-produced magnetized plasma with these properties. We characterize the diffusive transport of the particles experimentally. The results show that the transport is diffusive and that, for the regime of interest for the highest-energy cosmic rays, the diffusion coefficient is unaffected by the spatial intermittency of the magnetic field.

Role of collisionality and radiative cooling in supersonic plasma jet collisions of different materials

Physical Review E American Physical Society 101:2 (2020) 023205

Authors:

Collins, Valenzuela, Speliotopoulos, Aybar, Conti, Beg, Tzeferacos, Khiar, Gianluca Gregori

Abstract:

Currently there is considerable interest in creating scalable laboratory plasmas to study the mechanisms behind the formation and evolution of astrophysical phenomena such as Herbig-Haro objects and supernova remnants. Laboratory-scaled experiments can provide a well diagnosed and repeatable supplement to direct observations of these extraterrestrial objects if they meet similarity criteria demonstrating that the same physics govern both systems. Here, we present a study on the role of collision and cooling rates on shock formation using colliding jets from opposed conical wire arrays on a compact pulsed-power driver. These diverse conditions were achieved by changing the wire material feeding the jets, since the ion-ion mean free path (λmfp-ii) and radiative cooling rates (Prad) increase with atomic number. Low Z carbon flows produced smooth, temporally stable shocks. Weakly collisional, moderately cooled aluminum flows produced strong shocks that developed signs of thermal condensation instabilities and turbulence. Weakly collisional, strongly cooled copper flows collided to form thin shocks that developed inconsistently and fragmented. Effectively collisionless, strongly cooled tungsten flows interpenetrated, producing long axial density perturbations.

Fast magnetic reconnection in highly-extended current sheets at the National Ignition Facility

(2020)

Authors:

W Fox, DB Schaeffer, MJ Rosenberg, G Fiksel, J Matteucci, H-S Park, AFA Bott, K Lezhnin, A Bhattacharjee, D Kalantar, BA Remington, D Uzdensky, CK Li, FH Séguin, SX Hu

Potential of prompt γ-ray emission studies in fast-neutron induced fission: a first step

The European Physical Journal A Springer Nature 56:3 (2020) 98

Authors:

L Qi, C Schmitt, M Lebois, A Oberstedt, S Oberstedt, JN Wilson, A Al-Adili, A Chatillon, D Choudhury, A Gatera, G Georgiev, A Göök, B Laurent, A Maj, I Matea, SJ Rose, B Wasilewska, F Zeiser

Nonlinear plasma wavelength scalings in a laser wakefield accelerator

Physical Review E American Physical Society 101:2 (2020) 23209

Authors:

H Ding, A Döpp, M Gilljohann, J Götzfried, S Schindler, L Wildgruber, Gavin Cheung, Simon M Hooker, S Karsch

Abstract:

Laser wakefield acceleration relies on the excitation of a plasma wave due to the ponderomotive force of an intense laser pulse. However, plasma wave trains in the wake of the laser have scarcely been studied directly in experiments. Here we use few-cycle shadowgraphy in conjunction with interferometry to quantify plasma waves excited by the laser within the density range of GeV-scale accelerators, i.e., a few 10(18)cm−3. While analytical models suggest a clear dependency between the nonlinear plasma wavelength and the peak potential a0, our study shows that the analytical models are only accurate for driver strength a 0≲1. Experimental data and systematic particle-in-cell simulations reveal that nonlinear lengthening of the plasma wave train depends not solely on the laser peak intensity but also on the waist of the focal spot.