Abstract
It is shown that the magnitude of the Seebeck coefficient of a semiconductor has a maximum value that is close to one-half the energy gap divided by eT. An expression for the position of the Fermi level at which the Seebeck coefficient has a maximum or minimum value is derived, with account taken of the mobility and effective mass ratios. It is concluded that measurement of the Seebeck coefficient as a function of temperature on any novel semiconductor is one of the simplest ways of estimating its band gap.
Similar content being viewed by others
References
E. Müller, W. Heiliger, P. Reinshaus and H. Süssmann, to be published, Proc. 15th Intl. Conf. on Thermoelectrics, Pasadena, (1996).
Landolt-Bornstein, New Series III/22A.
M. Situmorang and H.J. Goldsmid, Proc. First European Conf. of Thermoelectrics, Cardiff, (1987), p. 135.
R.P. Chasmar and R. Stratton, J. Electronic Control 7, 52 (1959).
G. Mahan, J. Appl. Phys. 65, 1578 (1989).
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Goldsmid, H.J., Sharp, J.W. Estimation of the thermal band gap of a semiconductor from seebeck measurements. J. Electron. Mater. 28, 869–872 (1999). https://doi.org/10.1007/s11664-999-0211-y
Received:
Accepted:
Issue Date:
DOI: https://doi.org/10.1007/s11664-999-0211-y