Title | ||
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HSPICE macromodel of a Programmable Metallization Cell (PMC) and its application to memory design |
Abstract | ||
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This paper presents a new HSPICE macromodel of a Programmable Metallization Cell (PMC). The electrical characteristics of a PMC are simulated by using a geometric model that considers the vertical and lateral growth/dissolution of the metallic filament. The selection of the parameters is based on operational features, so the electrical characterization of the PMC is simple, easy to simulate and intuitive. The I-V and R-V plots of a PMC are generated at a very small error compared with experimental data; the proposed model also shows a small error for the relationship between the switching time and the pulse amplitude. The use of a PMC as resistive element in a crossbar memory is also presented; it is shown that a PMC-based crossbar offers substantial improvements over other resistive technologies. |
Year | DOI | Venue |
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2014 | 10.1109/NANOARCH.2014.6880477 | Nanoscale Architectures |
Keywords | Field | DocType |
SPICE,integrated circuit design,integrated circuit metallisation,integrated circuit modelling,random-access storage,CBRAM,HSPICE macromodel,I-V plots,PMC-based crossbar,R-V plots,conducting bridge random access memory,crossbar memory,electrical characteristics,geometric model,lateral growth-dissolution,memory design,metallic filament,parameter selection,programmable metallization cell,pulse amplitude,resistive element,switching time,vertical growth-dissolution,Conducting Bridge Random Access Memory (CBRAM),Emerging Technology,HSPICE,Modeling,Programmable Metallization Cell (PMC) | Switching time,Computer science,Resistive touchscreen,Geometric modeling,Electronic engineering,Programmable metallization cell,Pulse-amplitude modulation,Crossbar switch | Conference |
ISSN | Citations | PageRank |
2327-8218 | 3 | 0.46 |
References | Authors | |
2 | 3 |
Name | Order | Citations | PageRank |
---|---|---|---|
Pilin Junsangsri | 1 | 28 | 5.78 |
Fabrizio Lombardi | 2 | 1985 | 259.25 |
Jie Han | 3 | 863 | 66.92 |