2022
DOI: 10.1002/aelm.202200182
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A Deep Study of Resistance Switching Phenomena in TaOx ReRAM Cells: System‐Theoretic Dynamic Route Map Analysis and Experimental Verification

Abstract: two significant directions. First, it results in serious heat issues, which may jeopardize the life-time of circuits, and create dangerous positive feedback effects in the thermally-activated physical mechanisms, underlying the operating principles of certain devices. Concurrently, it leads to an inevitable upsurge in power consumption across a CMOS chip, which sheds shadows on the reliability of Dennard's law, [2] and prevents further increases in the clock frequency. Taking also into account the extremely-hi… Show more

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Cited by 20 publications
(4 citation statements)
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“…Thus, Δ x = 0 and eq are simplified to the following analytical expression: 0 T / 2 g false( prefix+ false) ( x ̅ s , v false( t false) ) .25em normald t 0em true︸ normalΔ x false( prefix+ false) prefix+ T / 2 T g false( prefix− false) ( x ̅ s , v false( t false) ) .25em normald t 0em true︸ normalΔ x false( prefix− false) = 0 The above equation allows calculation of the mean value x̅ s of the steady-state periodic oscillation in the memristor state x , for a predefined high-frequency periodic voltage input v ( t ). Importantly, eq describes the condition for the emergence of the fading memory phenomenon in memristors, based on which the steady-state time-response of the state variable x ( t ), depends on the characteristics of the voltage input v ( t ), but not on the initial memristor state x 0 (see Figure d, e). Through eq , the theoretical investigation performed in ref and ref provided a mathematical proof for the fading memory phenomenon in resistive switches that exhibit asymmetric switching kinetics with respect to the input polarity.…”
Section: Memristor Theorymentioning
confidence: 99%
“…Thus, Δ x = 0 and eq are simplified to the following analytical expression: 0 T / 2 g false( prefix+ false) ( x ̅ s , v false( t false) ) .25em normald t 0em true︸ normalΔ x false( prefix+ false) prefix+ T / 2 T g false( prefix− false) ( x ̅ s , v false( t false) ) .25em normald t 0em true︸ normalΔ x false( prefix− false) = 0 The above equation allows calculation of the mean value x̅ s of the steady-state periodic oscillation in the memristor state x , for a predefined high-frequency periodic voltage input v ( t ). Importantly, eq describes the condition for the emergence of the fading memory phenomenon in memristors, based on which the steady-state time-response of the state variable x ( t ), depends on the characteristics of the voltage input v ( t ), but not on the initial memristor state x 0 (see Figure d, e). Through eq , the theoretical investigation performed in ref and ref provided a mathematical proof for the fading memory phenomenon in resistive switches that exhibit asymmetric switching kinetics with respect to the input polarity.…”
Section: Memristor Theorymentioning
confidence: 99%
“…A theoretical tool to help in the analysis is the dynamic route map (DRM) (Chua (2018); Ascoli et al (2018); Marrone et al (2022)), which tracks the change of the state variable over time. This theoretical concept has already been successfully applied to describe the switching characteristics of ReRAMs (Maldonado et al (2020); Ascoli et al (2022)) and PCM (Marrone et al (2022)). In the deterministic view, the DRM (as the transition time) is independent of the initial value of the state variable.…”
Section: Linear Regimementioning
confidence: 99%
“…However, it should be mentioned that rather linear potentiation/depression characteristics can also be realized in filamentary switching devices if the pulse width meets the transition time of the switching event. [40,41]…”
Section: Potentiation and Depression Behaviormentioning
confidence: 99%