Electron transport properties of antimony doped SnO2 single crystalline thin films grown by plasma-assisted molecular beam epitaxy
J. Appl. Phys. 106, 093704 (2009); doi:10.1063/1.3254241
Published 6 November 2009
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By antimony doping tin oxide, SnO2:Sb (ATO), below 1.0% Sb concentration, controllable n-type doping was realized. Plasma-assisted molecular beam epitaxy has been used to grow high quality single crystalline epitaxial thin films of unintentionally doped (UID) and Sb-doped SnO2 on r-plane sapphire substrates. A UID thickness series showed an electron concentration of 7.9×1018 cm−3 for a 26 nm film, which decreased to 2.7×1017 cm−3 for a 1570 nm film, whereas the mobility increased from 15 to 103 cm2/V s, respectively. This series illustrated the importance of a buffer layer to separate unintentional heterointerface effects from the effect of low Sb doping. Unambiguous bulk electron doping was established by keeping the Sb concentration constant but changing the Sb-doped layer thickness. A separate doping series correlated Sb concentration and bulk electron doping. Films containing between 9.8×1017 and 2.8×1020 Sb atoms/cm3 generated an electron concentration of 1.1×1018–2.6×1020 cm−3. As the atomic Sb concentration increased, the mobility and resistivity decreased from 110 to 36 cm2/V s and 5.1×10−2 to 6.7×10−4
cm, respectively. The Sb concentration was determined by secondary ion mass spectrometry. X-ray diffraction and atomic force microscopy measurements showed no detrimental effects arising from the highest levels of Sb incorporation. Temperature dependent Hall measurements established a lower limit for the Sb electron activation energy of 13.2 meV and found that films with greater than 4.9×1019 electrons/cm3 were degenerately doped. Within experimental uncertainties, 100% donor efficiency was determined for Sb-doped SnO2 in the range studied.
©2009 American Institute of Physics
cm, respectively. The Sb concentration was determined by secondary ion mass spectrometry. X-ray diffraction and atomic force microscopy measurements showed no detrimental effects arising from the highest levels of Sb incorporation. Temperature dependent Hall measurements established a lower limit for the Sb electron activation energy of 13.2 meV and found that films with greater than 4.9×1019 electrons/cm3 were degenerately doped. Within experimental uncertainties, 100% donor efficiency was determined for Sb-doped SnO2 in the range studied.
©2009 American Institute of Physics
| History: | Received 22 July 2009; accepted 28 September 2009; published 6 November 2009 |
| Permalink: |
http://link.aip.org/link/?JAPIAU/106/093704/1 |
KEYWORDS and PACS
antimony,
atomic force microscopy,
buffer layers,
doping profiles,
electrical resistivity,
electron density,
electron mobility,
Hall effect,
molecular beam epitaxial growth,
plasma materials processing,
secondary ion mass spectra,
semiconductor doping,
semiconductor epitaxial layers,
semiconductor growth,
semiconductor materials,
tin compounds,
X-ray diffraction
- 73.61.Le
Electrical properties of other inorganic semiconductors (thin films) - 73.50.Jt
Galvanomagnetic and other magnetotransport effects in thin films - 68.37.Ps
Atomic force microscopy (AFM) of surfaces, interfaces and thin films - 79.20.Rf
Atomic, molecular and ion beam impact and interactions with surfaces - 73.50.Dn
Low-field transport and mobility; piezoresistance (thin films) - 52.77.-j
Plasma applications - 81.15.Hi
Molecular, atomic, ion, and chemical beam epitaxy - 61.72.up
Doping and impurity implantation in other materials - 68.55.ag
Semiconductor thin film nucleation and growth - YEAR: 2009
PUBLICATION DATA
0021-8979 (print)
1089-7550 (online)
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