4.4 Article

Thin film characterization of zinc tin oxide deposited by thermal atomic layer deposition

期刊

THIN SOLID FILMS
卷 556, 期 -, 页码 186-194

出版社

ELSEVIER SCIENCE SA
DOI: 10.1016/j.tsf.2014.01.068

关键词

Zinc tin oxide; Atomic layer deposition; Thin film; Transparent conductive oxide

资金

  1. Center for Nanostructuring for Efficient Energy Conversion, an Energy Frontier Research Center (EFRC)
  2. U.S. Department of Energy, Office of Science, Basic Energy Sciences (BES) [DE-SC0001060, DE-SC0004782]
  3. Bell Labs Graduate Fellowship Research Program
  4. Marcus and Amalia Wallenberg Foundation
  5. Academy of Finland [256800/2012]
  6. Finnish Cultural Foundation

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Zinc tin oxide (ZTO) thin films are of interest for many applications, including transparent conducting oxides and buffer layers in thin film solar cells. In this work, the ability of atomic layer deposition (ALD) to control both thickness and composition of the ternary material is explored and the resulting film properties are characterized. ZTO was deposited at 150 degrees C by alternating growth of tin oxide (SnOx) and zinc oxide (ZnO) using tetrakis(dimethylamido)tin and diethyl zinc as metal precursors and water as the oxygen source. The growth behavior of ZTO was systematically examined as a function of the relative fraction of SnOx to ZnO ALD cycles and their bilayer period. Variable angle spectroscopic ellipsometry (VASE) showed that the ZTO growth rate was strongly reduced as compared to the growth rates of the binaries, especially at low bilayer periods and low tin cycle fractions. Inductively-coupled plasma optical emission spectroscopy showed that the composition, together with other properties of ZTO films, was not simply proportional to the binary ALD cycle fractions utilized in the deposition. Structurally, the deposited films were shown by X-ray diffraction to be amorphous for tin content exceeding 10%, for which only smooth features were observed by scanning electron microscopy. Optically, VASE revealed a minimum refractive index in the visible range for intermediate compositions and a maximum for the pure SnOx phase. Conversely, the ZTO bandgap was maximized for intermediate metal compositions near similar to 50%, and converged to the direct ZnO bandgap of 3.3 eV for compositions with decreasing amounts of Sn in the films. Linear extrapolations gave a range of 2.9 to 4.0 eV for SnOx bandgap depending on the bandgap type (indirect or direct). (C) 2014 Elsevier B.V. All rights reserved.

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