Cultural advice

The Australian National University acknowledges, celebrates and pays our respects to the Ngunnawal and Ngambri people of the Canberra region and to all First Nations Australians on whose traditional lands we meet and work, and whose cultures are among the oldest continuing cultures in human history.

Aboriginal and Torres Strait Islander peoples are advised that ANU Library collections may include images, names, voices, and other representations of deceased persons.

Material in the collection may contain terms, language or views that reflect the period in which the item was created and may be considered inappropriate today.

Determining the band gap and mean kinetic energy of atoms from reflection electron energy loss spectra

Loading...
Thumbnail Image

Date

Authors

Vos, Maarten
Marmitt, G.G.
Finkelstein, Y
Moreh, R

Journal Title

Journal ISSN

Volume Title

Publisher

American Institute of Physics (AIP)

Abstract

Reflection electron energy loss spectra from some insulating materials (CaCO<inf>3</inf>, Li<inf>2</inf>CO<inf>3</inf>, and SiO<inf>2</inf>) taken at relatively high incoming electron energies (5-40 keV) are analyzed. Here, one is bulk sensitive and a well-defined onset of inelastic excitations is observed from which one can infer the value of the band gap. An estimate of the band gap was obtained by fitting the spectra with a procedure that includes the recoil shift and recoil broadening affecting these measurements. The width of the elastic peak is directly connected to the mean kinetic energy of the atom in the material (Doppler broadening). The experimentally obtained mean kinetic energies of the O, C, Li, Ca, and Si atoms are compared with the calculated ones, and good agreement is found, especially if the effect of multiple scattering is taken into account. It is demonstrated experimentally that the onset of the inelastic excitation is also affected by Doppler broadening. Aided by this understanding, we can obtain a good fit of the elastic peak and the onset of inelastic excitations. For SiO<inf>2</inf>, good agreement is obtained with the well-established value of the band gap (8.9 eV) only if it is assumed that the intensity near the edge scales as (E - E<inf>gap</inf>)1.5. For CaCO<inf>3</inf>, the band gap obtained here (7 eV) is about 1 eV larger than the previous experimental value, whereas the value for Li<inf>2</inf>CO<inf>3</inf> (7.5 eV) is the first experimental estimate.

Description

Keywords

Citation

Source

Journal of Chemical Physics

Book Title

Entity type

Access Statement

Open Access

License Rights

Restricted until