“…This nucleus decays into an excited state of 8 Be, which immediately breaks up into two α particles with energies around 1.6 MeV. Position-sensitive detectors for MeV α particles were already available, and allowed studies of the lattice sites of 8 Li in all of the semiconductors mentioned above, as a function of implantation temperature and, often also, for different types of doping [1,2,5,8,9,[12][13][14]. As a general feature it was found that following implantation at low temperatures Li preferred tetrahedral interstitial sites, while high-temperature implantation lead to the occupancy of substitutional sites in the III-V and II-VI semiconductors, and to bond-centered, substitutional or random sites in Si and Ge.…”