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Electron density dependence of the electronic structure of InN epitaxial layers grown on sapphire (0001)
42
Citations
26
References
2005
Year
The temperature dependence of the resistivity of InN was investigated as a function of carrier density. The carrier density was changed from ${n}_{e}=1.8\ifmmode\times\else\texttimes\fi{}{10}^{18}\phantom{\rule{0.3em}{0ex}}{\mathrm{cm}}^{\ensuremath{-}3}\phantom{\rule{0.3em}{0ex}}\text{to}\phantom{\rule{0.3em}{0ex}}1.5\ifmmode\times\else\texttimes\fi{}{10}^{19}\phantom{\rule{0.3em}{0ex}}{\mathrm{cm}}^{\ensuremath{-}3}$ by Si doping. The InN investigated showed metallic conduction above $20\phantom{\rule{0.3em}{0ex}}\mathrm{K}$. At lower temperatures there was a resistivity anomaly originating from carrier localization in the $a\text{\ensuremath{-}}b$ plane, which was confirmed by the magnetoresistance at $0.5\phantom{\rule{0.3em}{0ex}}\mathrm{K}$. The Shubnikov--de Haas oscillation showed that InN had a spherical Fermi surface and its radius increased according to the increase of ${n}_{e}$ when ${n}_{e}<5\ifmmode\times\else\texttimes\fi{}{10}^{18}\phantom{\rule{0.3em}{0ex}}{\mathrm{cm}}^{\ensuremath{-}3}$. In addition, an oscillation corresponding to the constant carrier density of $4.5\ifmmode\times\else\texttimes\fi{}{10}^{12}\phantom{\rule{0.3em}{0ex}}{\mathrm{cm}}^{\ensuremath{-}2}$ was observed in the field applied perpendicular to the $a\text{\ensuremath{-}}b$ plane. This oscillation showed an anomalous angle dependence on the magnetic field. Taking into account this density, we determined the critical carrier density of the Mott transition to be $2\ifmmode\times\else\texttimes\fi{}{10}^{17}\phantom{\rule{0.3em}{0ex}}{\mathrm{cm}}^{\ensuremath{-}3}$. Anisotropy of localization was observed within the $a\text{\ensuremath{-}}b$ plane, which indicates that the distribution of the electrons was not uniform in the $a\text{\ensuremath{-}}b$ plane. The ${n}_{e}$ dependence of the magnetoresistance revealed an electronic structure change around $5\ifmmode\times\else\texttimes\fi{}{10}^{18}\phantom{\rule{0.3em}{0ex}}{\mathrm{cm}}^{\ensuremath{-}3}$. From these results, an electronic structure at the fundamental absorption edge of InN grown on sapphire (0001) was presented.
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