Author: Anita Pokorska
The team of researchers from the Institute of
Plasma Physics and Laser Microfusion in Warsaw has performed systematic
numerical (particle-in-cell) studies of the properties of laser-driven
carbon ion beams produced under conditions relevant for ion fast
ignition (IFI) of DT fuel, and the feasibility of achieving beam
parameters required for IFI were discussed. The ignition of nuclear fuel
initiated by an intense laser-driven ion beam is a promising option of
Inertial Confinement fusion (ICF) which is currently one of the two main
paths towards an energy source based on thermonuclear fusion.
It
was found that a 1 ps 200 kJ infrared laser driver is capable of
producing ion beams with parameters required for IFI, even with a simple
non-optimised target, but only at small distances (<0.1 mm) from the
target. At such distances, the beam intensity and fluence exceeds 5 ×
1021 W cm−2 and 2 GJ cm−2,
respectively, while the beam energy approaches 30 kJ. The ion beam
parameters can be significantly improved by carefully selecting the
target thickness and shape. However, even with an optimised target,
achieving the beam parameters required for IFI is possible only at
distances from the target below 0.5 mm.
It was
shown for the first time that laser-accelerated heavy ion beams
produced under conditions relevant for IFI achieve higher parameters
determining fuel ignition than light ion or proton beams and, therefore,
may be more useful for IFI than previously thought.
The
ion acceleration is accompanied by the emission of powerful (>50 PW)
pulses of short-wavelength synchrotron radiation which are the source
of significant ion energy losses and may pose a threat to the fusion
infrastructure.
In addition to ICF, the
extremely intense ion beams can be a unique research tool for research
in nuclear physics, high energy-density physics or materials science.

The
intensity and the temporal shape of the ion pulse are two of the most
important characteristics of the ion beam that determine the fuel
ignition. These characteristics recorded at a distance x equal to 100
µm, 200 µm and 500 µm from the front of the target and averaged over the
area of aperture dap = 50 µm (the “useful part of the beam”)
for Li, C, Al, Ti and Cu ions are presented in figure. The highest peak
intensity and the shortest duration are achieved by the Cu ion pulse,
both in the near-expansion and far-expansion zone.