Controlled nuclear fusion initiated by highly intense laser beams has
been the subject of experiment for many years. The National Ignition F
acility (NIF) represents the culmination of design efforts to provide
a laser facility that will successfully demonstrate fusion ignition in
the laboratory. In this so-called inertial confinement approach, ener
getic driver beams (laser, X ray, or charged particle) heat the outer
surface of a spherical capsule containing deuterium and tritium (DT) f
uel. As the capsule surface explosively evaporates, reaction pressure
compresses the DT fuel causing the central core of the fuel to reach e
xtreme density and temperature. When the central temperature is high e
nough, DT fusion reactions occur. The energy released from these react
ions further heats the compressed fuel, and fusion burn propagates out
ward through the colder regions of the capsule much more rapidly than
the inertially confined capsule can expand. The resulting fusion react
ions yield many times more energy than was absorbed from the driver be
ams. Figure I summarizes the inertial confinement fusion (ICF) process
.