Abstract

Two sets of prominent photoluminescence (PL) lines, called A and B here, in electron-irradiated and ion-implanted $4H\text{-SiC}$ have been investigated by low-temperature PL microscopy. From their spectral details, temperature dependence, emission energies, introduction, and annealing characteristics it is concluded that they arise from the neutral on-axis and off-axis carbon antisite-vacancy pairs ${({\text{V}}_{\text{C}}{\text{C}}_{\text{Si}})}^{0}$. Photoluminescence excitation spectroscopy has been used to derive an energy-level diagram for the B set of lines of $4H\text{-SiC}$. The creation of these centers is demonstrated as a process that is sensitively dependent not only on the $n$ or $p$ doping of the material, as has been proposed but also on the temperature and the existence of inhomogeneous internal electric and strain fields. Samples of different purities from many different sources have been studied. Relatively impure, highly compensated doped samples exhibit very strong A and B PL and are referred to as AB material. Purer materials, largely uncompensated, called V here, that are $n(\text{N})$ or $p(\text{Al})$ doped, have photoluminescence from Si vacancy related defects but relatively little A or B intensity even after annealing at $900\text{ }\ifmmode^\circ\else\textdegree\fi{}\text{C}$. Similar sets of PL lines have also been observed in ion-implanted $4H\text{-SiC}$ and electron-irradiated $6H\text{-SiC}$ and investigated to a more limited extent. A wide range of different electron-irradiation conditions has been explored.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call