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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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Kyritsakis, Andreas
University of Tartu
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (10/10 displayed)
- 2024Polarization characteristics and structural modifications of Cu nanoparticles under high electric fields
- 2023Biased self-diffusion on Cu surface due to electric field gradientscitations
- 2023Critical review on experimental and theoretical studies of elastic properties of wurtzite-structured ZnO nanowirescitations
- 2022Thermal, Mechanical, and Acoustic Properties of Polydimethylsiloxane Filled with Hollow Glass Microspherescitations
- 2022Biased self-diffusion on Cu surface due to electric field gradientscitations
- 2020Tungsten migration energy barriers for surface diffusioncitations
- 2019Ab initio calculation of field emission from metal surfaces with atomic-scale defectscitations
- 2016Atomistic modeling of metal surfaces under high electric fieldscitations
- 2016Effects of control oxide material on the charging times of metal nanoparticles inside non-volatile memories
- 2016Extension of the general thermal field equation for nanosized emitterscitations
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article
Effects of control oxide material on the charging times of metal nanoparticles inside non-volatile memories
Abstract
<p>We have investigated the influence of different control oxide materials on the charging times of metal nanoparticles (mNP) inside a [Si/SiO2/(mNP)/Control-Oxide/gate] non-volatile memory (NVM) in which the control oxide can have a higher dielectric constant epsilon than that of SiO2 like HfO2 or Al2O3 as is the case in practice frequently. Our calculations are performed for both N-type and P-type substrates. We have used a previously published 3-dimensional Wentzel-Krammers-Brillouin (WKB) method of ours, which does not contain such adjustable parameters as effective area or capture cross-section which other 1-dimensional theories use. To obtain the total time for the charging of the NVM to saturation we calculate the times that successive electrons take to be incorporated into an mNP under a given applied voltage and a given duration of the charging pulse, each time updating the tunneling potential due to the incorporation of the extra electron into the mNP. We obtain an exponential dependence of these charging times on the dielectric constant of the control oxide for which we offer a simple explanation. The change with substrate type is on the other hand less pronounced. Our results are confirmed by experiment In particular, when our method is applied to NVMs with SiO2 and HfO2 as the control oxide we obtain good agreement with experiment without using such adjustable parameter as effective area of emission. We finally show that if the fraction of the substrate area that is covered with mNP is used to estimate this parameter the error involved will be quite significant, i.e. a factor of 5 approximately. (C) 2016 Elsevier B.V. All rights reserved.</p>