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-coupled memristive effect. Our model replicates eight types of characteristic nonlinear I-V behavior, which explains all observed nonpinched I-V curves seen in experiments. Furthermore, a reversible transition from a nonpinched I-V hysteresis loop to an ideal pinched I-V hysteresis loop is found, which explains the experimental data obtained in C15H11O6-based devices when subjected to an external stimulus (e.g., voltage, moisture, or temperature). Our results provide the vital physics models and materials insights for elucidating the origins of nonpinched I-V hysteresis loops ascribed to capacitive-coupled memristive behavior.
| Original language | English |
|---|---|
| Pages (from-to) | 6461-6465 |
| Number of pages | 5 |
| Journal | Nano Letters |
| Volume | 19 |
| Issue number | 9 |
| DOIs | |
| State | Published - 11 Sep 2019 |
| Externally published | Yes |
Keywords
- capacitive-coupled memristive
- current-voltage curve
- hysteresis loop
- nonpinched
- unified model
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