Präsentationsmaterialien
In this work, we analyze the energy loss of 4+ carbon projectiles at an energy of 0.6 MeV/u as they pass through a carbon plasma of the experiment to be carried out at GSI within the LIGHT (Laser Ion Generation, Handing and Transport) project. In this experiment, the aim is to measure the energy loss of carbon ions as they pass through a laser-generated carbon plasma. LIGHT provides ion pulse...
In TNSA-driven laser-plasma interaction, a crucial role is played by different sources of instabilities that can alter ion and proton acceleration in nominally identical conditions. Such instabilities can strongly affect the reproducibility of sequential shots.
The significative improvements in laser technology and in high repetition lasers, allow to investigate involved physical phenomena...
Double-Cone Ignition (DCI) is an innovative direct-drive scheme that employs oppositely placed gold cones to constrain the target shell assembly. Compared to spherical targets, DCI reduces the ns-laser irradiation solid angle, offering the potential for achieving implosion with lower driver energy. However, this requires a tailored irradiation scheme for DCI targets: the non-spherical geometry...
The transport process of intense ion beams in dense plasma is fundamentally relevant to high-energy-density physics, inertial confinement fusion, fast ignition, and related fields. In this study, the transportation behavior of laser-accelerated intense proton beam in a well-defined dense plasma(with a length L~1mm, temperature T~17eV, and electron density ne~4×1020cm-3) was measured. The...
The main challenge for efficient laser energy deposition in inertial confinement fusion (ICF) is stimulated laser scattering on plasma waves. Various optical laser beam smoothing techniques used over the years, such as random phase plates (RPP) and smoothing by spectral dispersion (SSD), appear inadequate for mitigating parametric instabilities. Following the success of ignition at the...
Important to the study of beam-driven inertial confinement fusion (ICF) as well as
Laser-accelerated ions typically exhibit an exponential energy spectrum up to a characteristic cut-off energy, which is a signature of target normal sheath acceleration (TNSA) [1]. However, many applications, such as proton therapy [2] or the fast ignition concept in inertial confinement fusion [3] benefit from well defined spectral shapes.
By introducing multiple ion species into the...