The α-emission channeling and blocking technique is a direct method for lattice site determination of radioactive atoms in single crystals. Position-sensitive detection of emitted α particles provides an efficient means of carrying out such experiments at very low doses (10 10 -10 11 implanted probe atoms per spectrum). Comparison of the experimental data to Monte Carlo simulations of complete twodimensional channeling patterns (e.g. ±2ϒ around <100>, <110> and <211> axes, which also includes all relevant planar directions) allows for straight-forward identification and rather accurate quantitative determination of occupied lattice sites, while at the same time the energy spectrum of emitted α particles gives information on the probe atom depth distribution.
AbstractThe α-emission channeling and blocking technique is a direct method for lattice site determination of radioactive atoms in single crystals. Position-sensitive detection of emitted α particles provides an efficient means of carrying out such experiments at very low doses (10 10 -10 11 implanted probe atoms per spectrum).Comparison of the experimental data to Monte Carlo simulations of complete two-dimensional channeling patterns (e.g. ±2ϒ around <100>, <110> and <211> axes, which also includes all relevant planar directions) allows for straight-forward identification and rather accurate quantitative determination of occupied lattice sites, while at the same time the energy spectrum of emitted α particles gives information on the probe atom depth distribution. We illustrate this for the case of ion implanted 8 Li (t _ =0.8 s) in Ge, where we identify mainly tetrahedral Li at room temperature, and bond-centered Li at slightly elevated temperature.