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Thickness effect of ultra-thin Ta(2)O(5) resistance switching layer in 28 nm-diameter memory cell
Resistance switching (RS) devices with ultra-thin Ta(2)O(5) switching layer (0.5–2.0 nm) with a cell diameter of 28 nm were fabricated. The performance of the devices was tested by voltage-driven current—voltage (I-V) sweep and closed-loop pulse switching (CLPS) tests. A Ta layer was placed beneath...
Autores principales: | , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group
2015
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4630583/ https://www.ncbi.nlm.nih.gov/pubmed/26527044 http://dx.doi.org/10.1038/srep15965 |
Sumario: | Resistance switching (RS) devices with ultra-thin Ta(2)O(5) switching layer (0.5–2.0 nm) with a cell diameter of 28 nm were fabricated. The performance of the devices was tested by voltage-driven current—voltage (I-V) sweep and closed-loop pulse switching (CLPS) tests. A Ta layer was placed beneath the Ta(2)O(5) switching layer to act as an oxygen vacancy reservoir. The device with the smallest Ta(2)O(5) thickness (0.5 nm) showed normal switching properties with gradual change in resistance in I-V sweep or CLPS and high reliability. By contrast, other devices with higher Ta(2)O(5) thickness (1.0–2.0 nm) showed abrupt switching with several abnormal behaviours, degraded resistance distribution, especially in high resistance state, and much lower reliability performance. A single conical or hour-glass shaped double conical conducting filament shape was conceived to explain these behavioural differences that depended on the Ta(2)O(5) switching layer thickness. Loss of oxygen via lateral diffusion to the encapsulating Si(3)N(4)/SiO(2) layer was suggested as the main degradation mechanism for reliability, and a method to improve reliability was also proposed. |
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