2015
DOI: 10.1109/ted.2015.2389832
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On the Origin of Steep $I$ –$V$ Nonlinearity in Mixed-Ionic-Electronic-Conduction-Based Access Devices

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Cited by 8 publications
(5 citation statements)
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“…It should be noted that the Cu ions were not uniformly distributed in the CuGeS layer (as observed from the Cu signal indicated by a solid green line), with a more enhanced intensity on interface than that in the body, implying the Cu ions tend to accumulate at the interface. This result is consistent with the results reported in Padilla's study, 37 where the metal ions of a MIEC material were found to have a U shape distribution in the metal-MIEC-metal structure at zero bias, with a higher concentration on the interface than in the center. This is a natural phenomenon of ion motion to keep a dynamic equilibrium between electrostatic ions drifting and diffusion.…”
Section: Results and Dissussionsupporting
confidence: 93%
“…It should be noted that the Cu ions were not uniformly distributed in the CuGeS layer (as observed from the Cu signal indicated by a solid green line), with a more enhanced intensity on interface than that in the body, implying the Cu ions tend to accumulate at the interface. This result is consistent with the results reported in Padilla's study, 37 where the metal ions of a MIEC material were found to have a U shape distribution in the metal-MIEC-metal structure at zero bias, with a higher concentration on the interface than in the center. This is a natural phenomenon of ion motion to keep a dynamic equilibrium between electrostatic ions drifting and diffusion.…”
Section: Results and Dissussionsupporting
confidence: 93%
“…7 can be explained by the size dependence of noise as in the RTN case [11], [13]. Here, bistable defects, namely, charged/uncharged point defects, such as oxygen vacancies [26], [27] or Cu impurities [28], close to the CF surface in LRS fluctuate between two different charge states, hence resulting in an intermittent depletion of carriers within the CF. As R increases, the CF becomes smaller, thus resulting in a transition from partial depletion at low R to full depletion at large R [11].…”
Section: Resistance Dependence Of Noisementioning
confidence: 99%
“…In TS devices, switching has been shown to originate from the motion of metallic ions and vacancies leading to a sharp increase in current, with switching voltage that depends on the material's band gap. 25 Interestingly, the same materials have been used as electrolytes across the different classes of resistance switching devices. For instance, copper-doped germanium sulfides and silicon dioxide have been demonstrated as effective electrolytes for application as both ECM and TS.…”
Section: ■ Introductionmentioning
confidence: 99%
“…By contrast, threshold switching is characterized by a diodelike I – V signal with an abrupt change in the resistance state of the device under an applied voltage. In TS devices, switching has been shown to originate from the motion of metallic ions and vacancies leading to a sharp increase in current, with switching voltage that depends on the material’s band gap . Interestingly, the same materials have been used as electrolytes across the different classes of resistance switching devices.…”
Section: Introductionmentioning
confidence: 99%