Editing Inertial confinement fusion (section)

==="High-energy" ICF===
High-energy ICF experiments (multi-hundred joules per shot) began in the early 1970s, when better lasers appeared. Funding for fusion research was stimulated by [[energy crisis|energy crises]] produced rapid gains in performance, and inertial designs were soon reaching the same sort of "below break-even" conditions of the best MCF systems.

LLNL was, in particular, well funded and started a laser fusion development program. Their [[Janus laser]] started operation in 1974, and validated the approach of using Nd:glass lasers for high power devices. Focusing problems were explored in the [[Long path laser|Long path]] and [[Cyclops laser]]s, which led to the larger [[Argus laser]]. None of these were intended to be practical devices, but they increased confidence that the approach was valid. It was then believed that a much larger device of the Cyclops type could both compress and heat targets, leading to ignition. This misconception was based on extrapolation of the fusion yields seen from experiments utilizing the so-called "exploding pusher" fuel capsule. During the late 1970s and early 1980s the estimates for laser energy on target needed to achieve ignition doubled almost yearly as plasma instabilities and laser-plasma energy coupling loss modes were increasingly understood. The realization that exploding pusher target designs and single-digit kilojoule (kJ) laser irradiation intensities would never scale to high yields led to the effort to increase laser energies to the 100 kJ level in the [[ultraviolet]] band and to the production of advanced ablator and cryogenic DT ice target designs.