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    Memristive Systems Analysis of

    3-Terminal Devices

    Blaise Mouttet

    ICECS 2010December 12-15Athens, Greece

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    Overview Review of Memristive, Mem-capacitive, and Mem-

    inductive Systems

    Introduction to Mem-Transistor Systems Small signal analysis of Mem-Transistor Systems

    Examples

    Widrow-Hoff memistor

    Synaptic floating gate transistor Nano-ionic MOSFET

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    Memristive Systems Resistive dynamic system

    defined by a state vector x

    v= R(x,i,t)i

    dx/dt = f(x,i,t)

    Degenerates to linearresistor at high frequency(property 6)

    Examples of memristive

    behavior was originallynoted from thermistor,neural models anddischarge tubes.

    L.O. Chua, S.M. Kang. Memristive Devices and Systems, Proceedings of the IEEE,

    Vol. 64, iss.2 (1976)

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    In 1967 Argall demonstrated

    zero-crossing resistancehysteresis and frequencydependence for thin film TiO2.

    F.Argall Switching Phenomena in Titanium Oxide Thin Films, Solid-State Electronics,

    Vol. 11, pp.535-541 (1968).

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    Mem-capacitive Systems Capacitive dynamic

    system defined by astate vector xq= C(x,v,t)v

    dx/dt = f(x,v,t) Degenerates to linear

    capacitor at highfrequency

    Examples of mem-capacitive behavior arefound in nanocrystaland perovskite thinfilms

    M. DiVentra, Y. V. Pershin, L.O. Chua, Putting Memory into Circuit Elements:

    Memristors, Memcapacitors, and Meminductors, Proceedings of the IEEE,vol 97, iss.8,(2009)

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    Mem-inductive Systems Inductive dynamic

    system defined by astate vector x

    f= L(x,i,t)i

    dx/dt = f(x,i,t)

    Degenerates to linearinductor at highfrequency

    Examples of mem-inductive behavior arefound in MEMSinductors

    Y. V. Pershin, M. DiVentra, Memory effects in complex materials and nanoscalesystems, arXiv:submit/0144853 (2010)

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    Transistor = Transfer Resistor

    (can amplify signals but is memory-less)

    Memristor = Memory Resistor(has memory but dissipates signal energy)

    Is it possible to build a singular non-linearcircuit element having features of both a

    memristor and a transistor?

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    2-Port Model of Voltage-Controlled

    Transistor

    I1 = g(V1,V2)I2= h(V1,V2)

    I1 = Y11V1+Y12V2I2= Y21V1+Y22V2

    Small signallinearization

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    2-Port Model of Voltage-Controlled

    Mem-Transistor

    I1 = g(V1,V2,x)I2= h(V1,V2,x)dx/dt =f(V1,V2,x)

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    TransconductanceIn the LaPlace domain the transconductance is determinedfrom the small signal linearization. System stability is determined

    by the sign of

    g

    0g0

    0g0

    g

    0g00g0

    g

    dm

    v)x,h(V

    x

    )x,f(Vs

    v

    )x,f(V

    x

    )x,h(V

    (s)V(s)Ig

    x

    )x,f(V 0g0

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    Transconductance

    g

    0g0

    0g0

    g

    0g00g0

    g

    d

    m v

    )x,h(V

    x

    )x,f(Vj

    v

    )x,f(V

    x

    )x,h(V

    (s)V

    (s)I

    g

    For periodic excitation frequencies (s=jw) the transconductanceof a mem-transistor is generally a frequency dependent complexnumber and represents both gain and a phase shift between

    the input and output signals.

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    Transconductance

    g

    0g0

    0g0

    g

    0g00g0

    g

    d

    m v

    )x,h(V

    x

    )x,f(Vj

    v

    )x,f(V

    x

    )x,h(V

    (s)V

    (s)I

    g

    At high excitation frequencies (w) the first term reducesto zero and the transconductance reduces to that of an ordinarytransistor.

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    Examples

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    Example #1:Widrow-Hoff Memistor

    B. Widrow, An Adaptive ADALINE Neuron Using Chemical Memistors, Stanford

    Electronics Laboratories Technical Report 1553-2, October 1960.

    In 1960 a 3-terminalelectrochemicalmemistor was

    developed by BernardWidrow and MarcianHoff.

    The memistor formeda central componentto an early ANN andthe development ofthe LMS algorithm.

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    Example #1:Widrow-Hoff Memistor

    B. Widrow, An Adaptive ADALINE Neuron Using Chemical Memistors, Stanford

    Electronics Laboratories Technical Report 1553-2, October 1960.

    The memistor was experimentally shown to demonstrate acharge- dependent conductance in a similar fashion to thelater predicted memristor of Chua.

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    Example #2: Synaptic Transistor

    C.Diorio,P.Hasler,B.A.Minch,C.A.Mead, A single-transistor silicon synapse, IEEE

    Transactions on Electron Devices, Vol. 43, No. 11, Nov. 1996.

    Since the 1990sanalog floating gateMOSFET transistors

    have been designed toact as synapses forneuromorphichardware.

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    Example #2: Synaptic Transistor

    C.Diorio,P.Hasler,B.A.Minch,C.A.Mead, A single-transistor silicon synapse, IEEE

    Transactions on Electron Devices, Vol. 43, No. 11, Nov. 1996.

    VVdc

    Vm

    d

    VVdc

    V

    Vgc

    V

    VbiVdg

    V

    bidgg

    VVdc

    V

    Vgc

    V

    Tcorner

    ewi

    weeVVi

    ew

    Qww

    ww

    dt

    dw

    1

    )(

    2

    2

    0

    2

    2

    1

    1

    max

    The sub-thresholdmodeling equationsdeveloped by Diorio et

    al. represent a 1st

    order, voltage-controlled mem-transistor with thestate variable equal tothe source current and

    Vgc as the controlvoltage.

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    Example #3: Nano-ionic FET

    D.B. Strukov, G.S. Snider, D.R. Stewart, R.S. Williams The missing memristor found,

    Nature, Vol. 453, May 2008.

    Nano-ionic motion of oxygenvacancies in TiO2/TiO2-x hasbeen used by Strukov et al. to

    explain memristive effects. If TiO2 thickness > tunneling

    gap then memcapacitiveeffects would be expected as a

    result of ionic drift.

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    Example #3: Nano-ionic FET

    2kT

    w)a,qE(Vsinhfae

    dt

    dw

    (w)V

    V1(w)VV

    2L

    WC(w)I

    0.5VV(w)VVLWC(w)I

    n(w)kT

    qV(w)expII

    GCU/kT

    A

    DS2

    TGSnd

    2DSDSTGSnd

    GS0d sub-threshold region

    saturationregion

    triode region

    Ionic drift equation:

    Long channel MOSFET equations:

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    N-port Memory Resistive Systems

    I1 = g1(V1,V2,..,Vn,x)I2= g2(V1,V2,..,Vn,x)

    .

    .In= gn(V1,V2,..,Vn,x)

    dx/dt =f(V1,V2,..,Vn,x)

    B.Mouttet Memristive Transfer Matrices, arXiv:1004:0041 (2010)

    B.Mouttet Programmable Crossbar Signal Processor, U.S. Patent 7 302 513, (2007)

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    Summary Mem-transistor systems analysis has been proposed based

    on non-linear, dynamic 2-port systems. A generalized transconductance of mem-transistors

    includes both gain and phase shift and may be useful todetermining mem-transistor stability.

    Some 3-terminal electronic devices have been shown toexhibit memory effects over the past 50 years but thetransistor models have rarely included non-linear dynamicsystems analysis.

    In addition to memristors, memcapacitors, andmeminductors, mem-transistors will likely play anincreasingly important role in 21st century electronics toachieve neuromorphic and bio-inspired computing.