2014
DOI: 10.1109/ted.2014.2341274
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An Analytical Model for the Forming Process of Conductive-Bridge Resistive-Switching Random-Access Memory

Abstract: An analytical model for the forming process of conductive-bridge resistive-switching random-access memory is developed. The measurable forming time can be calculated using this model giving the biasing condition and is verified to be correct through comparison with the experimental data. The forming time has been shown to have multiple-slopes in exponential dependence on the applied voltage, in agreement with measurement. The model is based on the identification of three steps in the forming process: 1) metal … Show more

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Cited by 7 publications
(5 citation statements)
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“…Furthermore, in AgI a large amount of Ag ion interstitials is already available within the film and a counter charge is not required. Thus, an initial injection of Ag ions and a migration through the complete insulator thickness, which has been taken into account by other groups, 43 is not required.…”
Section: Simulation Proceduresmentioning
confidence: 99%
“…Furthermore, in AgI a large amount of Ag ion interstitials is already available within the film and a counter charge is not required. Thus, an initial injection of Ag ions and a migration through the complete insulator thickness, which has been taken into account by other groups, 43 is not required.…”
Section: Simulation Proceduresmentioning
confidence: 99%
“…18,19 Recent experiments 17,20,21 on the nanoscale metallic clusters in dielectrics indicate complicate electrochemical mechanism to determine the filament growth in CBRAM. Some simulation works about filament growth have been reported, [22][23][24][25] the physical mechanism of filament growth in the atomistic level is still need to be clarified. In this paper, we quantitatively demonstrate two types of filament growth using KMC and appropriate model parameters.…”
mentioning
confidence: 99%
“…5e ). The formation of an oxygen-rich crystalline shell is attributed to a combined effect of temperature and lateral motion of , which is dominated by two opposite forces: inwards thermal diffusion driven by a temperature gradient and outwards Fickian diffusion driven by a concentration gradient 59 61 (see Supplementary Fig. 8 ).…”
Section: Resultsmentioning
confidence: 99%