Hostname: page-component-5c6d5d7d68-xq9c7 Total loading time: 0 Render date: 2024-08-22T05:12:08.718Z Has data issue: false hasContentIssue false

Extension of the Constant Photocurrent Method to Determine Densities of Occupied and Unoccupied Localised States

Published online by Cambridge University Press:  21 March 2011

Charlie Main
Affiliation:
University of Abertay Dundee, School of Computing and Advanced Technologies, Bell Street, Dundee DD1 1HG
Steve Reynolds
Affiliation:
University of Abertay Dundee, School of Computing and Advanced Technologies, Bell Street, Dundee DD1 1HG
Ivica Zrinŝcak
Affiliation:
University of Abertay Dundee, School of Computing and Advanced Technologies, Bell Street, Dundee DD1 1HG
Amar Merazga
Affiliation:
Faculté des Sciences et Sciences de l'ingénieur, Université Mohammed Khidir, Biskra, Algéria
Get access

Abstract

This paper examines the use of Constant Photocurrent (CPM) measurements on thin film semiconductors, employing steady (DC) and modulated (AC) sub-gap illumination, to determine the density of localised states (DOS) in the bandgap. AC and DC measurements often result in different apparent absorption spectra. It is demonstrated that it is possible not only to extract information from the respective 'absorption' spectra, on the DOS below the Fermi level - i.e. occupied states, but also on the density of unoccupied states above the Fermi level. The ability to discriminate between these two groups of states by using DC and AC modulated sub-gap light arises from the frequency dependence of the different excitation pathways by which free electrons can be produced. AC modulated excitation will reveal absorption associated with transitions from occupied states into the conduction band, while DC excitation will include transitions from the valence band into unoccupied defect states, followed by slow thermal emission to the conduction band. We examine the temperature dependence of the CPM spectra and present a simple analysis of the DC and AC absorption spectra which allows the two regions of the DOS, above and below the Fermi level, to be determined.

Type
Research Article
Copyright
Copyright © Materials Research Society 2004

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

REFERENCES

1. Main, C., Reynolds, S., Zrinŝcak, I. and Merazga, A. 2003, Mat. Res. Soc. Symp. Proc. 762,(2003) 131136 Google Scholar
2. Sládek, P. and Thèye, M. L., Solid State Comms. 89 (1994) 199 Google Scholar
3. Hasegawa, S., Nitta, S. and Nonomura, S., J. Non-Cryst. Solids 198–200 (1996) 544.Google Scholar
4. Conte, G., Irrera, F., Nobile, G. and Palma, F., J. Non-Cryst. Solids 164–166 (1993) 419.Google Scholar
5. Pierz, K., Mell, H. and Terukov, J., J. Non-Cryst. Solids 97–98, (1985) 547.Google Scholar
6. Vanecek, M., Abrahám, A., Ŝtika, O., Stuchlík, J. and Kocka, J., Phys. Stat. Sol. (a) 83 (1984), 617.Google Scholar
7. Jensen, P., Solid State Comm. 76, (1990), 1301 Google Scholar
8. Main, C., Reynolds, S., and Zrinŝcak, I., J. Materials Science: Materials in Electronics. 14 (2003) 681684 Google Scholar