We report on shadowgraphic measurements showing the first space-and time-resolved snapshots of ultraintense laser pulse-generated fast electrons propagating through a solid target. A remarkable result is the formation of highly collimated jets (,20-mm) traveling at the velocity of light and extending up to 1 mm. This feature clearly indicates a magnetically assisted regime of electron transport, of critical interest for the fast ignitor scheme. Along with these jets, we detect a slower (ഠc͞2) and broader (up to 1 mm) ionization front consistent with collisional hot electron energy transport. 52.60. + h The fast ignitor scheme, which claims to relax some of the constraints hampering the standard approaches to inertial confinement fusion, has triggered a worldwide interest since its inception [1]. It hinges on the rapid additional heating of the core of a precompressed thermonuclear pellet due to the slowing down of a bunch of relativistic electrons generated by an ultraintense laser pulse. Now, the highly overcritical plasma surrounding the core should prevent any laser pulse from reaching it, whatever highintensity penetration mechanisms are at work (relativistic self-induced transparency [2] or ponderomotive hole boring [3]). An encouraging point is that particle-in-cell simulations predict a rather peaked hot electron distribution in the vicinity of the laser-solid interaction zone [4]. However, an efficient heating of the core requires the electron beam to remain collimated up to its final absorption zone, i.e., on a distance of several hundreds of microns. This can be achieved only through the pinching effect of the beam-driven magnetic field competing with multiple scattering. Therefore, fast electron transport from moderately to extremely dense regions appears as a key issue for the success of fast ignition, which must be thoroughly tackled both experimentally and theoretically.Over the past year, there has been a growing body of experimental evidence pointing to the existence of very collimated high intensity laser-produced electron jets traveling through solid targets. Tatarakis et al. have recently observed a narrow expanding plasma at the rear surface of thick plastic slabs irradiated by a 1 ps, 10 19 W͞cm 2 laser pulse [5]. By using a 2D Fokker-Planck hybrid code, they interpreted this localized rear heating as a magnetic field-enhanced electron energy deposition at the target/vacuum interface [6]. This effect has also been detected in other experiments [7]. Though very encouraging, these studies still provide an incomplete experimental picture of the phenomena arising in the bulk of the target.In the present paper, we report on optical shadowgraphic results showing what is, to our knowledge, the first comprehensive set of space-and time-resolved snapshots of fast electrons propagating through a solid target. In order to bypass the classical limitation of optical probing into an overcritical solid target, we use transparent glass slides. Our measurements pinpoint the existence of two types of fast...
Fast electron generation and propagation were studied in the interaction of a green laser with solids. The experiment, carried out with the LULI TW laser (350 fs, 15 J), used K(alpha) emission from buried fluorescent layers to measure electron transport. Results for conductors (Al) and insulators (plastic) are compared with simulations: in plastic, inhibition in the propagation of fast electrons is observed, due to electric fields which become the dominant factor in electron transport.
Experiments of heating of solid targets by fast electrons have been analyzed by means of simulations with a recently developed hybrid code. Electron propagation, refluxing effects, relative importance of self-generated fields, and heating of targets are presented. We found a good agreement between simulations and experiments on the Kα yield.
We study the propagation of fast electrons in a gas at different densities. A large relativistic electron current is produced by focusing a short-pulse ultrahigh-intensity laser on a metallic target. It then propagates in a gas jet placed behind the foil. Shadowgraphy in the gas shows an electron cloud moving at sub-relativistic average velocities. The experiment shows (i) the essential role of the density of background material for allowing propagation of fast electrons, (ii) the importance of the ionization phase which produces free electrons available for the return current, and (iii) the effect of electrostatic fields on fast-electron propagation.
The propagation of relativistic electrons in foam and solid density targets has been studied by means of K-alpha spectroscopy. Experimental results point out the role of self-generated electric fields in propagation and the role of heating of matter induced by the passage of fast electrons. A simple analytical formulation has been given and Spitzer conductivity has been shown to be fairly compatible with experimental results.
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