Abstract
Other authors in this book have discussed at length the applications and synthesis of transparent conducting oxides (TCOs). Our purpose in this chapter is to discuss some elementary aspects of TCO properties, which can be explained surprisingly well using the Drude free-electron theory [1]. Although this theory explains the electrical properties and fits the optical data so well, many have questioned whether any fundamental understanding of TCOs can be gained from its use. We believe that much can be learned about the properties of the conduction electrons in some, but not all, TCOs. The conduction electrons are important because they dominate the optical properties of the materials in the visible and near-infrared (NIR) wavelengths. The functional form of the free-electron theory often accounts for measurable properties of TCOs such as transmittance and reflectance, and their relationship to extrinsically controllable properties (e.g., carrier concentration and relaxation time) and intrinsic, uncontrollable, properties (e.g., crystal lattice and effective mass,).
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Notes
- 1.
This can be shown from the second of Newton’s equations of motion, \( s = 1/2a{t^2} \). We put \( \bar{a} = e\bar{E}/m ^* \) and \( t = 1/2f \), where \( f = \omega /2\pi. \) For a wavelength of 1.5µm, an effective mass of 0.35m e and an electric field strength of 1Vm−1, the amplitude, s, is about 2×10−7nm. Even though the electric field strength is assumed to be constant, this approach is sufficient to make an order of magnitude estimate. If we include scattering of the electrons, then an estimate of the amplitude may be made from (3.7). With a mobility of 50cm2V−1s−1, and the same conditions as above, the amplitude is about 4×10−8nm.
- 2.
For a typical plasma wavelength of 1.5µm, an effective mass of 0.35m e, and a relaxation time of about 5×10−15s, corresponding to a mobility of about 25cm2V−1s−1, this inequality is obeyed to within about 2.5%. It is obeyed to better than 10% over the full range of frequencies shown in Fig.3.2.
- 3.
The Fresnel reflection coefficient is given by \( R = \frac{{{{\left( {N - 1} \right)}^2} + {k^2}}}{{{{\left( {N + 1} \right)}^2} + {k^2}}} \). Hence, at low frequency, where both N and k are relatively large, the reflection coefficient is also large.
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Acknowledgements
This work was performed under U.S. Department of Energy contract number DE-AC36-GO9910337. The authors would like to express their thanks for the input given by Yuki Yoshida (now of Sanyo) and Viktor Kaydanov (formerly of the Colorado School of Mines).
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Coutts, T.J., Young, D.L., Gessert, T.A. (2011). Modeling, Characterization, and Properties of Transparent Conducting Oxides. In: Ginley, D. (eds) Handbook of Transparent Conductors. Springer, Boston, MA. https://doi.org/10.1007/978-1-4419-1638-9_3
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