Abstract:Historically, there has been a controversy regarding whether the leakage current versus voltage (I-V) relationship is governed by the Schottky mechanism or by the Poole-Frenkel (P-F) mechanism for several decades. For the P-F mechanism, the I-V characteristics is expected to be symmetrical. In this paper, the author points out that there is an extra mechanism for symmetrical I-V characteristics.
“…For example, this was discussed by Lau in 2012. 24 For a semiconductor p-n junction, the forward characteristics can be represented by a small forward voltage V F such that the current through the p-n junction is very large when the bias voltage is above V F while the current is zero when the bias voltage is below V F . For a silicon p-n junction, V F is about 0.7 V. Similarly, for a metal/semiconductor Schottky barrier, the forward I-V characteristics can be characterized by a small forward voltage V F ; V F is usually smaller for a Schottky diode compared to a p-n junction diode.…”
Section: Theorymentioning
confidence: 99%
“…The author believes that the results from Yamaguchi et al and Aleskandrova et al can be understood if an assumption is made that their ZrO 2 /SiO 2 /Si interfacial region had a very large quantity of defect states. According to Lau 2012, 24 a very large quantity of defect states, which may originate from the interaction between ZrO 2 and Si during ZrO 2 deposition and subsequent processing, make the effective Schottky barrier height lower and also insensitive to the choice of metal (for this case, n + -Si or p + -Si). It can be imagined that the Al gate was deposited at near room temperature and the interaction between Al and ZrO 2 at low processing temperature is not as strong as that between ZrO 2 and Si at high processing temperature and the effective Schottky barrier height at the Al/ZrO 2 interface is higher than that at the ZrO 2 /SiO 2 /Si interfacial region.…”
Historically, there is a controversy regarding the current-voltage (I-V) characteristics of thin film MIM (metal-insulator-metal) capacitors, which is quite frequently modeled by either the Schottky model or the Poole-Frenkel model. In this paper, the author points out that the two models actually can be unified. The physics underlying this model involves a non-uniform distribution of deep donor defect states such that a very large quantity of defect states exist at the two interface of the MIM capacitor while the density of defect states in the insulator bulk is relatively low, resulting in an M/n-i-n/M structure. This unified Schottky-Poole-Frenkel model can be further extended to include other effects like space charge limited current and tunneling. The effect of trap limited space charge limited current is also discussed. Examples of the application of this theory will be provided for MIM capacitors based on various high-k dielectric materials like tantalum oxide, titanium oxide, zirconium oxide and aluminum oxide.
“…For example, this was discussed by Lau in 2012. 24 For a semiconductor p-n junction, the forward characteristics can be represented by a small forward voltage V F such that the current through the p-n junction is very large when the bias voltage is above V F while the current is zero when the bias voltage is below V F . For a silicon p-n junction, V F is about 0.7 V. Similarly, for a metal/semiconductor Schottky barrier, the forward I-V characteristics can be characterized by a small forward voltage V F ; V F is usually smaller for a Schottky diode compared to a p-n junction diode.…”
Section: Theorymentioning
confidence: 99%
“…The author believes that the results from Yamaguchi et al and Aleskandrova et al can be understood if an assumption is made that their ZrO 2 /SiO 2 /Si interfacial region had a very large quantity of defect states. According to Lau 2012, 24 a very large quantity of defect states, which may originate from the interaction between ZrO 2 and Si during ZrO 2 deposition and subsequent processing, make the effective Schottky barrier height lower and also insensitive to the choice of metal (for this case, n + -Si or p + -Si). It can be imagined that the Al gate was deposited at near room temperature and the interaction between Al and ZrO 2 at low processing temperature is not as strong as that between ZrO 2 and Si at high processing temperature and the effective Schottky barrier height at the Al/ZrO 2 interface is higher than that at the ZrO 2 /SiO 2 /Si interfacial region.…”
Historically, there is a controversy regarding the current-voltage (I-V) characteristics of thin film MIM (metal-insulator-metal) capacitors, which is quite frequently modeled by either the Schottky model or the Poole-Frenkel model. In this paper, the author points out that the two models actually can be unified. The physics underlying this model involves a non-uniform distribution of deep donor defect states such that a very large quantity of defect states exist at the two interface of the MIM capacitor while the density of defect states in the insulator bulk is relatively low, resulting in an M/n-i-n/M structure. This unified Schottky-Poole-Frenkel model can be further extended to include other effects like space charge limited current and tunneling. The effect of trap limited space charge limited current is also discussed. Examples of the application of this theory will be provided for MIM capacitors based on various high-k dielectric materials like tantalum oxide, titanium oxide, zirconium oxide and aluminum oxide.
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