Author :
Fedosejevs, R ; Higginson, DP ; Friesen, H ; Sorokovikova, A ; Jarrott, LC ; Link, A ; Kemp, GE ; Hey, D ; Ping, Y ; Bush, I ; Beaudry, A ; Tait, J ; Westwood, J.N. ; Tiedje, HF ; Singh, S ; Mo, MZ ; Tsui, YY ; Westover, B ; Beg, FN ; Akli, KU ; Freeman,
Abstract :
Summary form only given. Fast Ignition [1] holds the promise of improved efficiency and reduced laser energy requirements for Laser Fusion Energy systems. The main approach proposed to date is by coupling a beam of 1 to 2 MeV electrons from the laser interaction spot to a 40 micron spot in the compressed fuel core using a metal cone insert to get close to the compressed core [2]. However, multi-millijoule level laser prepulse can create extended preplasmas within the cone, effectively moving the electron generation source region far back from the cone tip and core [3]. By employing second harmonic pulses much reduced levels of prepulse can be achieved and at the same time colder electron distribution can be obtained, closer to those required ultimately for Fast Ignition.