| CONDENSED MATTER: ELECTRONIC STRUCTURE, ELECTRICAL, MAGNETIC, AND OPTICAL PROPERTIES |
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On the Voltage and Frequency Distribution of Dielectric Properties and ac Electrical Conductivity in Al/SiO2/p-Si (MOS) Capacitors |
| Ahmet Kaya*, Şemsettin Altındal, Yasemin Şafak Asar, Zekayi Sönmez |
Department of Physics, Faculty of Sciences, Gazi University, 06500, Ankara, Turkey
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| Cite this article: |
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Ahmet Kaya, &Scedil, emsettin Alt?ndal et al 2013 Chin. Phys. Lett. 30 017301 |
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Abstract An Al/SiO2/p-Si (MOS) capacitor with a thick (826 ?) interfacial oxide layer (SiO2) which is formed by using the thermal oxidation method is fabricated to investigate both frequency and applied bias voltage dependences of real and imaginary parts of dielectric constant (ϵ' and ϵ") and electric modulus (M' and M"), loss tangent (tanδ) and ac electrical conductivity (σac) in a wide frequency range from 1 kHz to 1 MHz at room temperature. The dielectric properties of the MOS capacitor are obtained using the forward and reverse bias capacitance-voltage (C–V) and conductance-voltage (G/ω–V) measurements in the applied bias voltage range 1.4–5.6 V. The values of ϵ', ϵ", tanδ, M', M" and σac are found to be strong functions of frequency and applied bias voltage in the depletion region due to excess capacitance Cex and conductance Gex/ω especially at low frequencies. The experimental results show that the interfacial polarization can occur at low frequencies more easily, consequently contributing to the dispersion in ϵ', ϵ", tanδ, M', M" and σac values of the MOS capacitor. The other reason for dispersion in the dielectric properties may be attributed to a particular density distribution of interface states (Nss) localized at the Si/SiO2 interface, as well as space charge carriers and inhomogeneity of interfacial oxide layer. The increase in conductivity with increasing frequency can be attributed to the hopping type conduction mechanism. It can be concluded that the ϵ', ϵ", tanδ, M', M" and σac values of the Al/SiO2/p-Si (MOS) capacitor are strongly dependent on both the frequency and applied bias voltage especially in the depletion region.
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Received: 18 July 2012
Published: 04 March 2013
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| PACS: |
73.40.Qv
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(Metal-insulator-semiconductor structures (including semiconductor-to-insulator))
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77.22.Ch
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(Permittivity (dielectric function))
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72.20.-i
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(Conductivity phenomena in semiconductors and insulators)
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