Bonding in alpha-quartz (SiO2): A view of the unoccupied states

High-resolution core-loss and low-loss spectra of alpha-quartz were acquire d by electron energyloss spectroscopy (EELS) with a transmission electron m icroscope (TEM). Spectra contain the Si L-1, L-2,L-3, K, and O K core-loss edges, and the surface and bulk low-loss spectra. The core-loss edges repre sent the atom-projected partial densities of states of the excited atoms an d provide information on the unoccupied s, p, and d states as a function of energy above the edge onset. The band structure and total density of state s were calculated for alpha-quartz using a self-consistent pseudopotential method. Projected local densities of Si and O s, p, and d states (LDOS) wer e calculated and compared with the EELS core-loss edges. These LDOS success fully reproduce the dominant Si and O core-loss edge shapes up to ca. 15 eV above the conduction-band onset. In addition, the calculations provide evi dence for considerable charge transfer From Si to O and suggest a marked io nicity of the Si-O bond. The experimental and calculated data indicate that O 2p-Si d pi-type bonding is minimal. The low-loss spectra exhibit four pe aks that are assigned to transitions from maxima in the valence-band densit y of states to the conduction band. A band gap of 9.65 eV is measured from the low-loss spectrum. The structures of the surface low-loss spectrum are reproduced by the joint density of states derived from the band-structure c alculation. This study provides a detailed description of the unoccupied DO S of alpha-quartz by comparing the core-loss edges and low-loss spectrum, o n a relative energy scale and relating the spectral features to the atom- a nd angular-momentum-resolved components of a pseudopotential band-structure calculation.