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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Ohno, H.
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (25/25 displayed)
- 2018Spin transport and spin torque in antiferromagnetic devicescitations
- 2017Magnetic domain-wall creep driven by field and current in Ta/CoFeB/MgOcitations
- 2016Fermi level position, Coulomb gap, and Dresselhaus splitting in (Ga,Mn)Ascitations
- 2010Anomalous Hall effect in field-effect structures of (Ga,Mn)Ascitations
- 2010Curie temperature versus hole concentration in field-effect structures of Ga1-xMnxAscitations
- 2008Prefacecitations
- 20080.7 anomaly and magnetotransport of disordered quantum wirescitations
- 2007Character of states near the Fermi level in (Ga,Mn)As: Impurity to valence band crossovercitations
- 2007Domain wall resistance in perpendicularly magnetized (Ga,Mn) Ascitations
- 2006Velocity of domain-wall motion induced by electrical current in the ferromagnetic semiconductor (Ga,Mn)Ascitations
- 2006Domain-wall resistance in ferromagnetic (Ga,Mn)Ascitations
- 2004Magnetotransport properties of metallic (Ga,Mn)As films with compressive and tensile straincitations
- 2003Ferromagnetic III-V and II-VI semiconductorscitations
- 2003Spin degree of freedom in ferromagnetic semiconductor hetero structurescitations
- 2003Modeling and simulation of polycrystalline ZnO thin-film transistorscitations
- 2002Control of ferromagnetism in field-effect transistor of a magnetic semiconductorcitations
- 2002Ferromagnetism of magnetic semiconductors: Zhang-Rice limitcitations
- 2002chapter 1 III-V Ferromagnetic Semiconductorscitations
- 2001Spin polarization dependent far infrared absorption in Ga1-xMnxAscitations
- 2001Hole-mediated ferromagnetism in tetrahedrally coordinated semiconductorscitations
- 2001Ferromagnetism in III-V and II-VI semiconductor structurescitations
- 2000Ferromagnetism induced by free carriers in p-type structures of diluted magnetic semiconductorscitations
- 2000Electric-field control of ferromagnetismcitations
- 2000Magnetotransport properties of (Ga,Mn)As investigated at low temperature and high magnetic fieldcitations
- 2000Zener model description of ferromagnetism in zinc-blende magnetic semiconductorscitations
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article
Modeling and simulation of polycrystalline ZnO thin-film transistors
Abstract
<jats:p>Thin-film transistors (TFTs) made of transparent channel semiconductors such as ZnO are of great technological importance because their insensitivity to visible light makes device structures simple. In fact, there have been several demonstrations of ZnO TFTs achieving reasonably good field effect mobilities of 1–10 cm2/V s, but the overall performance of ZnO TFTs has not been satisfactory, probably due to the presence of dense grain boundaries. We modeled grain boundaries in ZnO TFTs and performed simulation of a ZnO TFT by using a two-dimensional device simulator in order to determine the grain boundary effects on device performance. Polycrystalline ZnO TFT modeling was started by considering a single grain boundary in the middle of the TFT channel, formulated with a Gaussian defect distribution localized in the grain boundary. A double Schottky barrier was formed in the grain boundary, and its barrier height was analyzed as a function of defect density and gate bias. The simulation was extended to TFTs with many grain boundaries to quantitatively analyze the potential profiles that developed along the channel. One of the main differences between a polycrystalline ZnO TFT and a polycrystalline Si TFT is that the much smaller nanoscaled grains in a polycrystalline ZnO TFT induces a strong overlap of the double Schottky barriers with a higher activation energy in the crystallite and a lower barrier potential in the grain boundary at subthreshold or off-state region of its transfer characteristics. Through the simulation, we were able to estimate the density of total trap states localized in the grain boundaries for polycrystalline ZnO TFT by determining the apparent mobility and grain size in the device.</jats:p>