2012 4th IEEE International Memory Workshop 2012
DOI: 10.1109/imw.2012.6213627
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Study of One Dimension Thickness Scaling on Cu/HfOx/Pt Based RRAM Device Performance

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Cited by 2 publications
(7 citation statements)
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“…At the filament center, the maximum local temperature T max = 729 K is measured with V a = 0.6 V and r f = 5 nm. The obtained T max , above the critical temperature T Crit = 600 K for the HfO 2 RRAM device, is adequate to contribute to resistive switching Figure (a) illustrates the complete voltage sweep as a function of time, whereas Figure (b) demonstrates the calculated local temperature on a time scale, with a maximum local temperature of 729 K in the positive bias domain and 400 K in the negative bias domain, consistent with the reported work …”
Section: Device Modelsupporting
confidence: 86%
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“…At the filament center, the maximum local temperature T max = 729 K is measured with V a = 0.6 V and r f = 5 nm. The obtained T max , above the critical temperature T Crit = 600 K for the HfO 2 RRAM device, is adequate to contribute to resistive switching Figure (a) illustrates the complete voltage sweep as a function of time, whereas Figure (b) demonstrates the calculated local temperature on a time scale, with a maximum local temperature of 729 K in the positive bias domain and 400 K in the negative bias domain, consistent with the reported work …”
Section: Device Modelsupporting
confidence: 86%
“…In this section, the analytically calculated resistive switching event from the device model is compared with the power signature calculated from experimental data, illustrated in Figure . The conductivity of the filament remains constant throughout the SET switching (HRS → LRS), while the filament radius varies . On the other hand, the filament conductivity varies while the radius remains constant during RESET switching (LRS → HRS) .…”
Section: Device Modelmentioning
confidence: 99%
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“…However, as the final transition metal oxide (TMO) thickness in CRRAM is controlled via selective etching during contact hole formation, CRRAM is subject to a large variation effect during mass production [35][36]. It is well known that the TMO thickness is one of the key parameters in an RRAM device that critically affects the basic resistive switching characteristics such as the set/reset time, operating voltage1, and low/high resistance states [37][38][39][40]. CRRAM reported in previous studies [33][34] was subject to nonuniformity in TMO thicknesses across an array To better control the overall TMO thickness in RRAM devices and improve the yield rate of RRAM characteristics by previous fabrication process, in this study, a new process flow of forming a TMO film by backfilling SiO 2 with plasma-…”
Section: Introductionmentioning
confidence: 99%