Memory Transistors
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Transcript of Memory Transistors
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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.