Optical properties of SnO2 thin films grown by atmospheric pressure chemical vapour deposition oxiding SnCl4

Abstract Tin oxide thin films were grown by chemical vapour deposition (CVD) on glass substrates at atmospheric pressure (AP) and temperatures varying between 350 and 520 °C. A vertical home-made reactor was used for the deposition from SnCl4 vapours with ambient air as oxidizer. Optical transmission measurements of these films were taken in the spectral range 200–2000 nm, and were analysed with the aid of the physical model introduced by Forouhi and Bloomer describing the optical dispersion in amorphous dielectrics ( A. Foroubi and I. Bloomer, Phys. Rev. B, 34 (1986) 7018 ). It was found that the model describes well the optical properties of APCVD SnO2 thin films. The structure and the composition of the films changed with the deposition temperature and these changes implied modifications in the optical and electrical properties. Hence, the increase in the deposition temperature was found to imply an increase in the energy distance between bonding and antibonding states and a decrease in the energy band gap, as defined by the physical model. Energy states were found to appear within the energy gap as the deposition temperature increased. These states were related to the enhanced film conductivities.

[1]  R. Ghoshtagore,et al.  Mechanism of CVD Thin Film SnO2 Formation , 1978 .

[2]  Robert H. Rediker,et al.  Electrical Properties of High‐Quality Stannic Oxide Crystals , 1971 .

[3]  V. Vasu,et al.  Physical properties of sprayed SnO2 films , 1991 .

[4]  John D. Mackenzie,et al.  Sol-gel-derived tin oxide thin films , 1995 .

[5]  Bloomer,et al.  Optical dispersion relations for amorphous semiconductors and amorphous dielectrics. , 1986, Physical review. B, Condensed matter.

[6]  K. H. Jolliffee Optical properties of thin solid films , 1954 .

[7]  W. Kern,et al.  Chemical Vapor Deposition of Transparent, Electrically Conductive Tin Oxide Films Formed from Dibutyl Tin Diacetate , 1975 .

[8]  F. G. Peters,et al.  Devitrification of Tin Oxide Films (Doped and Undoped) Prepared by Reactive Sputtering , 1965 .

[9]  W. Spence The uv Absorption Edge of Tin Oxide Thin Films , 1967 .

[10]  R. Summitt,et al.  The ultraviolet absorption edge of stannic oxide (SnO2) , 1964 .

[11]  R. Helbig,et al.  Growth of SnO2 single crystals by a vapour phase reaction method , 1976 .

[12]  R. Berjoan,et al.  Morphology of SnO2 thin films obtaibed by the sol-gel technique , 1994 .

[13]  N. J. Chou,et al.  Chemical Composition and Electrical Properties of Tin Oxide Films Prepared by Vapor Deposition , 1973 .

[14]  V. Dutta,et al.  Electrical and optical properties of undoped and antimony‐doped tin oxide films , 1980 .

[15]  J. Gasiot,et al.  Thermally stimulated emission from traps and related problems in SnO2 monocrystals , 1970 .

[16]  J. Melsheimer,et al.  Band gap energy and Urbach tail studies of amorphous, partially crystalline and polycrystalline tin dioxide , 1985 .

[17]  J. Houston,et al.  Photoelectronic Analysis of Imperfections in Grown Stannic Oxide Single Crystals , 1965 .

[18]  Emil Wolf,et al.  Principles of Optics: Contents , 1999 .

[19]  N. Mott,et al.  Electronic Processes In Non-Crystalline Materials , 1940 .

[20]  S. H. Liu,et al.  The effect of mercury UV photolysis on vapour deposition of SnO2 , 1992 .