8 research outputs found
Space-filling, multi-fractal, localized thermal spikes in silicon, germanium and zinc oxide
The mechanism responsible for the emission of clusters from heavy ion
irradiated solids is proposed to be thermal spikes. Collision cascade-based
theories describe atomic sputtering but cannot explain the consistently
observed experimental evidence for significant cluster emission. Statistical
thermodynamic arguments for thermal spikes are employed here for qualitative
and quantitative estimation of the thermal spike-induced cluster emission from
silicon, germanium and zinc oxide. The evolving cascades and spikes in
elemental and molecular semiconducting solids are shown to have fractal
characteristics. Power law potential is used to calculate the fractal
dimension.The fractal dimension is shown to be dependent upon the exponent of
the power law interatomic potential. Each irradiating ion has the probability
of initiating a space-filling, multi-fractal thermal spike that may sublime a
localized region near the surface by emitting clusters in relative ratios that
depend upon the energies of formation of respective surface vacancies.Comment: 16 pages, 6 figure
Status of Wakefield Monitor Experiments at the CLIC Test Facility
For the very low emittance beams in CLIC, it is vital to mitigate emittance growth which leads to reduced luminosity in the detectors. One factor that leads to emittance growth is transverse wakefields in the accelerating structures. In order to combat this the structures must be aligned with a precision of a few um. For achieving this tolerance, accelerating structures are equipped with wakefield monitors that measure higher-order dipole modes excited by the beam when offset from the structure axis. We report on such measurements, performed using prototype CLIC accelerating structures which are part of the module installed in the CLIC Test Facility 3 (CTF3) at CERN. Measurements with and without the drive beam that feeds rf power to the structures are compared. Improvements to the experimental setup are discussed, and finally remaining measurements that should be performed before the completion of the program are summarized