FIGURE 2. The coupled variable-resistor model for a memristor.

From the following article:

The missing memristor found

Dmitri B. Strukov, Gregory S. Snider, Duncan R. Stewart & R. Stanley Williams

Nature 453, 80-83(1 May 2008)

doi:10.1038/nature06932

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a, Diagram with a simplified equivalent circuit. V, voltmeter; A, ammeter. b, c, The applied voltage (blue) and resulting current (green) as a function of time t for a typical memristor. In b the applied voltage is v0sin(omega0t) and the resistance ratio is Unfortunately we are unable to provide accessible alternative text for this. If you require assistance to access this image, or to obtain a text description, please contact npg@nature.com, and in c the applied voltage is plusminusv0sin2(omega0t) and Unfortunately we are unable to provide accessible alternative text for this. If you require assistance to access this image, or to obtain a text description, please contact npg@nature.com, where v0 is the magnitude of the applied voltage and omega0 is the frequency. The numbers 1–6 label successive waves in the applied voltage and the corresponding loops in the i–v curves. In each plot the axes are dimensionless, with voltage, current, time, flux and charge expressed in units of v0 = 1 V, Unfortunately we are unable to provide accessible alternative text for this. If you require assistance to access this image, or to obtain a text description, please contact npg@nature.com, t0 equivalent to 2pi/omega0 equivalent to D2/muVv0 = 10 ms, v0t0 and i0t0, respectively. Here i0 denotes the maximum possible current through the device, and t0 is the shortest time required for linear drift of dopants across the full device length in a uniform field v0/D, for example with D = 10 nm and muV = 10-10 cm2 s-1 V-1. We note that, for the parameters chosen, the applied bias never forces either of the two resistive regions to collapse; for example, w/D does not approach zero or one (shown with dashed lines in the middle plots in b and c). Also, the dashed i–v plot in b demonstrates the hysteresis collapse observed with a tenfold increase in sweep frequency. The insets in the iv plots in b and c show that for these examples the charge is a single-valued function of the flux, as it must be in a memristor.

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