By David S. Ginley, John D. Perkins (auth.), David S. Ginley (eds.)
Transparent engaging in fabrics are key parts in a large choice of present applied sciences together with flat panel monitors, photovoltaics, natural, low-e home windows and electrochromics. the wishes for brand new and greater fabrics is urgent, as the latest fabrics do not need the functionality degrees to satisfy the ever- expanding call for, and since the various present fabrics used will not be potential sooner or later. furthermore, the sector of obvious conductors has undergone dramatic alterations within the final 5-7 years with new fabrics being pointed out, new purposes and new humans within the box. “Handbook of obvious Conductors” provides obvious conductors in a ancient point of view, presents present functions in addition to insights into the way forward for the units. it's a finished reference, and represents the most up-tp-date source at the subject.
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Additional resources for Handbook of Transparent Conductors
The conduction band dispersions in GGA are correct. Thus, once corrected for the error, the band structures shown are correct. There are a number of methods beyond LDF which do give better band gaps. The best known of these is the GW method , but this is computationally very expensive. Other popular methods are the self-interaction correction (SIC)  and the B3LYP functional [33–35]. B3LYP is a hybrid functional, that is a LDFtype functional of the exchange-correlation energy containing a fraction of the Hartree-Fock function, which can give the correct total energy and reasonable eigenvalues.
Kawazoe, Journal of Non-Crystalline Solids 203, 334–344 (1996). 76. G. Granqvist, Solar Energy Materials and Solar Cells 60, 201–262 (2000). 77. K. H. E. R. A. M. Branz, Electrochimica Acta 46, 2125–2130 (2001). 78. G. Granqvist (1995). Handbook of Inorganic Electrochromic Materials. Amsterdam, Elsevier. 79. D. W. Teplin, M. L. Alleman, X. S. M. M. S. Ginley, Y. Lin and Y. Lu, Applied Surface Science 223, 124–132 (2004). 80. “Highly conductive epitaxial CdO thin films prepared by pulsed laser deposition”, M.
The indirect band gap has been adjusted to the experimental value. The bands are very similar to those given by Ingram et al. . The other important calculations of CuAlO2 are by Yanagi  and Zhang . We see that 3R-CuAlO2 is an indirect gap semiconductor. The conduction band minimum is at G and consists of Cu s states, while the valence band maximum is at F. The upper valence band from 0 eV down to À8 eV consists of a mixture of Cu d and O 2p states, with the Cu d states tending to lie higher.