2019
DOI: 10.1021/acs.nanolett.9b02683
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A Unified Capacitive-Coupled Memristive Model for the Nonpinched Current–Voltage Hysteresis Loop

Abstract: The concept of the memristor, a resistor with memory, was proposed by Chua in 1971 as the fourth basic element of electric circuitry. Despite a significant amount of effort devoted to the understanding of memristor theory, our understanding of the nonpinched current–voltage (I–V) hysteresis loop in memristors remains incomplete. Here we propose a physical model of a memristor, with a capacitor connected in parallel, which explains how the nonpinched I–V hysteresis behavior originates from the capacitive-couple… Show more

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Cited by 153 publications
(87 citation statements)
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“…[ 16 ] Recently, a capacitive‐coupled memristive effect has been suggested to illustrate the nonpinched current–voltage ( I – V ) hysteresis loop based on a model of parallel connecting an ideal memristor and capacitor. [ 17 ] It also implies the feasible coexistence of the functions of the memristor and solid supercapacitor in principle.…”
Section: Introductionmentioning
confidence: 99%
“…[ 16 ] Recently, a capacitive‐coupled memristive effect has been suggested to illustrate the nonpinched current–voltage ( I – V ) hysteresis loop based on a model of parallel connecting an ideal memristor and capacitor. [ 17 ] It also implies the feasible coexistence of the functions of the memristor and solid supercapacitor in principle.…”
Section: Introductionmentioning
confidence: 99%
“…When the bias exceeds 3 V, the device exhibits a symmetric resistive switching performance at high bias while the contribution of the capacitive response remained at low bias (Figure b,e and Figures S1c and S2c, Supporting Information). This implies that the single TiO 2 nanobelt device changes from a capacitive behavior to a capacitive‐coupled memristor behavior when the sweeping bias exceeds 3 V. The capacitive‐coupled memristive effect has been previously reported in the case of nonvolatile memory devices, but, to the best of our knowledge, this is the first time that this characteristic has been reported in volatile threshold switching devices . Further increasing the sweeping bias up to 10 V (Figure c,f) and 20 V (Figures S2i and S3i, Supporting Information) will lead to an increased current for the resistive switching behavior, but the devices still have a small capacitive contribution at low bias.…”
Section: Resultsmentioning
confidence: 55%
“…This implies that the single TiO 2 nanobelt device changes from a capacitive behavior to a capacitive-coupled memristor behavior when the sweeping bias exceeds 3 V. The capacitive-coupled memristive effect has been previously reported in the case of nonvolatile memory devices, [47] but, to the best of our knowledge, this is the first time that this characteristic has been reported in volatile threshold switching devices. [48] Further increasing the sweeping bias up to 10 V (Figure 3c,f) and 20 V (Figures S2i and S3i, Supporting Information) will lead to an increased current for the resistive switching behavior, but the devices still have a small capacitive contribution at low bias. This is why the I-V curve of the TiO 2 nanobelt device is not pinched to zero, in great contrast to the zero-crossing behavior typically observed in memristive devices.…”
Section: I-v Sweeping Performance and Transport Mechanism Studymentioning
confidence: 99%
“…Because of the unique advantages and potential applicability of biomemristors, biomemristors have a wide range of applications in electronic skin, biomedical and brain chip applications. [ 3,4 ] In general, biomemristor cells must be biocompatible and for electronic applications. [ 5–7 ] However, most memristor cells are made of inorganic materials, which are brittle and incompatible without flexible and versatile functionalities.…”
Section: Introductionmentioning
confidence: 99%