The fourth element: characteristics, modelling and electromagnetic theory of the memristor by O....

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The fourth element: characteristics, modelling and electromagnetic theory of the memristor by O. Kavehei, A. Iqbal, Y. S. Kim, K. Eshraghian, S. F. Al-Sarawi, and D. Abbott Proceedings A Volume 466(2120):2175-2202 August 8, 2010 ©2010 by The Royal Society

Transcript of The fourth element: characteristics, modelling and electromagnetic theory of the memristor by O....

Page 1: The fourth element: characteristics, modelling and electromagnetic theory of the memristor by O. Kavehei, A. Iqbal, Y. S. Kim, K. Eshraghian, S. F. Al-Sarawi,

The fourth element: characteristics, modelling and electromagnetic theory of the memristor

by O. Kavehei, A. Iqbal, Y. S. Kim, K. Eshraghian, S. F. Al-Sarawi, and D. Abbott

Proceedings AVolume 466(2120):2175-2202

August 8, 2010

©2010 by The Royal Society

Page 2: The fourth element: characteristics, modelling and electromagnetic theory of the memristor by O. Kavehei, A. Iqbal, Y. S. Kim, K. Eshraghian, S. F. Al-Sarawi,

The four fundamental two-terminal circuit elements.

O. Kavehei et al. Proc. R. Soc. A 2010;466:2175-2202

©2010 by The Royal Society

Page 3: The fourth element: characteristics, modelling and electromagnetic theory of the memristor by O. Kavehei, A. Iqbal, Y. S. Kim, K. Eshraghian, S. F. Al-Sarawi,

Schematic of HP MR, where D is the device channel length and w is the length of the doped region.

O. Kavehei et al. Proc. R. Soc. A 2010;466:2175-2202

©2010 by The Royal Society

Page 4: The fourth element: characteristics, modelling and electromagnetic theory of the memristor by O. Kavehei, A. Iqbal, Y. S. Kim, K. Eshraghian, S. F. Al-Sarawi,

Two MRs in series: (a) with the same polarity, both η=−1 or both η=+1; (b) with opposite polarities, η=−1 and η=+1.

O. Kavehei et al. Proc. R. Soc. A 2010;466:2175-2202

©2010 by The Royal Society

Page 5: The fourth element: characteristics, modelling and electromagnetic theory of the memristor by O. Kavehei, A. Iqbal, Y. S. Kim, K. Eshraghian, S. F. Al-Sarawi,

The hysteresis of an MR based on equation (2.16).

O. Kavehei et al. Proc. R. Soc. A 2010;466:2175-2202

©2010 by The Royal Society

Page 6: The fourth element: characteristics, modelling and electromagnetic theory of the memristor by O. Kavehei, A. Iqbal, Y. S. Kim, K. Eshraghian, S. F. Al-Sarawi,

The hysteresis characteristics of the MR. It shows that the memristance value is varying from a very low to a very high resistance.

O. Kavehei et al. Proc. R. Soc. A 2010;466:2175-2202

©2010 by The Royal Society

Page 7: The fourth element: characteristics, modelling and electromagnetic theory of the memristor by O. Kavehei, A. Iqbal, Y. S. Kim, K. Eshraghian, S. F. Al-Sarawi,

The hysteresis characteristics using the nonlinear drift assumption.

O. Kavehei et al. Proc. R. Soc. A 2010;466:2175-2202

©2010 by The Royal Society

Page 8: The fourth element: characteristics, modelling and electromagnetic theory of the memristor by O. Kavehei, A. Iqbal, Y. S. Kim, K. Eshraghian, S. F. Al-Sarawi,

Nonlinear window functions, (a) F(x)=1−(2x−1)2p, (b) F(x)=1−(x− sgn(−i))2p.

O. Kavehei et al. Proc. R. Soc. A 2010;466:2175-2202

©2010 by The Royal Society

Page 9: The fourth element: characteristics, modelling and electromagnetic theory of the memristor by O. Kavehei, A. Iqbal, Y. S. Kim, K. Eshraghian, S. F. Al-Sarawi,

The SPICE macro-model of MR. Here, G, H and S are a VCCS, CCVS, and a switch (VON=−1.9 V and VOFF=−2 V), respectively.

O. Kavehei et al. Proc. R. Soc. A 2010;466:2175-2202

©2010 by The Royal Society

Page 10: The fourth element: characteristics, modelling and electromagnetic theory of the memristor by O. Kavehei, A. Iqbal, Y. S. Kim, K. Eshraghian, S. F. Al-Sarawi,

The MR characteristics.

O. Kavehei et al. Proc. R. Soc. A 2010;466:2175-2202

©2010 by The Royal Society

Page 11: The fourth element: characteristics, modelling and electromagnetic theory of the memristor by O. Kavehei, A. Iqbal, Y. S. Kim, K. Eshraghian, S. F. Al-Sarawi,

The MR characteristics when a step input voltage is applied.

O. Kavehei et al. Proc. R. Soc. A 2010;466:2175-2202

©2010 by The Royal Society

Page 12: The fourth element: characteristics, modelling and electromagnetic theory of the memristor by O. Kavehei, A. Iqbal, Y. S. Kim, K. Eshraghian, S. F. Al-Sarawi,

The MR characteristics when (i) a 1 kHz sinusoidal voltage is applied.

O. Kavehei et al. Proc. R. Soc. A 2010;466:2175-2202

©2010 by The Royal Society

Page 13: The fourth element: characteristics, modelling and electromagnetic theory of the memristor by O. Kavehei, A. Iqbal, Y. S. Kim, K. Eshraghian, S. F. Al-Sarawi,

The I–V curves for (a) two MRs in parallel, (b) two MRs in series and (c) a single MR. In all of the cases, there is no difference between an MR and equivalent resistor in the network.

O. Kavehei et al. Proc. R. Soc. A 2010;466:2175-2202

©2010 by The Royal Society

Page 14: The fourth element: characteristics, modelling and electromagnetic theory of the memristor by O. Kavehei, A. Iqbal, Y. S. Kim, K. Eshraghian, S. F. Al-Sarawi,

Step voltage response curves for (i) (R) resistor–memristor, (ii) (C) capacitor–memristor and (iii) (L) inductor–memristor.

O. Kavehei et al. Proc. R. Soc. A 2010;466:2175-2202

©2010 by The Royal Society

Page 15: The fourth element: characteristics, modelling and electromagnetic theory of the memristor by O. Kavehei, A. Iqbal, Y. S. Kim, K. Eshraghian, S. F. Al-Sarawi,

MR-op-amp integrator circuit and its response to the input step voltage.

O. Kavehei et al. Proc. R. Soc. A 2010;466:2175-2202

©2010 by The Royal Society