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(1)

Ella Gale, Ben de Lacy

Costello and Andrew

Adamatzky

The Effect of Electrode Size on

Memristor Properties: An

(2)

A.

Which Model of

Memristance Works

Best

B.

What Effect

Electrode Size has

on Memristor

Properties

(3)
(4)

M

= memristance

q

= charge

φ

= magnetic flux

CHUA’S

(5)

1.

Strukov et al’s

Phenomenalogical Model

2.

Georgiou et al’s Bernoulli

Equations

3.

Mem-Con Model

There Are Three Theoretical Memristor

Models

(6)

1. Phenomenological

Model

𝑀

(

𝑞

(

𝑡

)

)

=𝑅off 𝜇𝑣

𝐷2 𝑅off 𝑅on 𝑞(𝑡 )

Strukov et al, The Missing Memristor Found, Nature, 2008

= ionic mobility of the O+

vacancies

Roff = resistance of TiO2

Ron = resistance of TiO(2-x)

(7)

Rewrote Strukov et al’s model as

Bernoulli Equations

Gained Some Analytical Solutions

Predicts the Size of the Hysteresis, ,

in Memristor I-V curves

(8)

= ‘Dimensionless Lumped Parameter’

Contains:

‘all’ physical dimensions of device

all parameters of experiment

is related to

is related to

The Model Predictions

2. GEORGIOU ET AL’S MODEL

~

𝛽

=

2

𝛽

=

2

𝑉

𝑚𝑎𝑥

𝜔

0

𝑅

02

𝜇

𝑣

(

𝑅

𝑜𝑛

𝐷

)

2

(

𝑅

𝑜𝑓𝑓

𝑅

𝑜𝑛

1

)

(9)

Universal constants:

, Experimental constants: product of

surface area () and electric field (),

, Material variable, =, where

3. Memristance, as Derived from Ion

Flow

Gale, The Missing Magnetic Flux in the HP Memristor Found, 2011

(10)

𝑀

𝑒

=

𝐶

𝑀

𝑀

+

𝐶

2

𝑅

𝐶𝑜𝑛

=

(

𝐷

𝑤

(

𝑡

)

)

𝜌

𝑜𝑓𝑓

𝐸𝐹

Memory Function Conservation Function

MEM-CON MODEL

(11)

Goal: To Investigate Which Theoretical Model Works Best Method:

A. Spatial Dimension Effects (Strukov and Mem-Con)

B. Test Hysteresis Predicitons (Georgiou)

(12)

• Strukov et al’s suggests no effect of size of E or F

• Georgiou et al suggest no effect of E or F

• Mem-Con model suggests that changing E or F will affect memristance

• Test whether there is an effect of altering E or F

(13)

Our Memristors

Crossed

Aluminium

electrodes

Thin-film (40nm)

TiO

2

sol-gel layer

E = 4mm

F = 1, 2, 3, 4 or

5mm

1. Gergel-Hackett et al, A Flexible Solution Processed Memristor, IEEE Elec. Dev. Lett., 2009

(14)

Pictures

Curved (BPS -like) Memristors

Triangular (UPS -like) Memristors

(15)

The Effect of

Varying Electrode Size

(16)
(17)
(18)

As , ,

Fit Memory Function to as a function of

(19)

Memory function Describes

’s variation with F

(20)

CONSERVATION FUNCTION DESCRIBES ’S VARIATION WITH F

(21)

• Measured and vary with electrode size

• This relationship is well described by the Mem-Con theory

• Hysteresis is effected by Electrode Size

• The Mem-Con Theory Correctly Predicts that

Memristance Should be a Function of the Three Spatial Dimensions

• The Strukov Theory Incorrectly Asserts that it is Only a Function of 1 Spatial Dimenion

(22)

Is the Hysteresis Related

to the ‘dimensionless

lumped parameter’, ?

(23)

THE EXAMPLE GIVEN IN GEORGIOU ET AL’S PAPER

(24)
(25)
(26)
(27)

• Georgiou et al’s Bernoulli Equation Formulation does not work at predicting hysteresis*

• Electrode Size can be changed to control hysteresis size*

• The Mem-Con Model can be used to predict which electrode sizes will give a certain max or min resistance

value (at the same omega)*

• All three spatial dimensions of the memristor are important in describing memristance

• The Mem-Con Model is a good model for real world memrstors

* For Curved Type Devices (see next talk for an explanation)

(28)

Ella Gale, Ben de Lacy

Costello and Andrew

Adamatzky

FILAMENTARY EXTENSION OF THE

MEM-CON THEORY OF

MEMRISTANCE AND ITS

(29)

Pictures

Curved (BPS -like) Memristors

Triangular (UPS -like) Memristors

(30)
(31)
(32)

Extend the Mem-Con

Model to Describe

Filamentary

(Triangular)

Memristors

(33)
(34)

φ

q

V

I

(35)

What the Flux?

𝑑 𝜑

=

𝑀

(

𝑞

(

𝑡

)

)

𝑑𝑞

𝑀

(

𝑞

(

𝑡

)

)

=

𝑅

𝑜𝑓𝑓

𝜇

𝑣

𝐷

2

𝑅

𝑜𝑓𝑓

𝑅

𝑜𝑛

𝑞

(

𝑡

)

But, where is the magnetic flux?

𝑉

=

𝑀

(

𝑡

)

𝐼

(36)

The Mem-Con model is based on calculating the MAGNETIC FLUX of the IONS for several reasons:

The IONS are the memory property, i.e. they hold the state

of the memristor

The IONS move slower than the electrons and it is this that

causes both the lag (hysteresis) and frequency response

The ION mobility, , is the physical quantity that controls

the dynamics of the system

Therefore, using magnetostatics to calculate the relationships between the ionic magnetic flux and charge we will arrive at a formula for memristance that satisfies Chua’s definition

(37)

Mem-Con Theory

𝑞

𝑀(𝑞 )

𝜑

𝑉

𝑅

𝑡𝑜𝑡

(𝑡)

𝐼

Ionic

Electronic

(38)
(39)
(40)

EQUIVALENT CIRCUIT DIAGRAM TO THE DEVICE

CHEMISTRY

𝑅𝑇𝑜𝑡(𝑡)= 1

1

(

𝑅𝑢+𝑀𝑒(𝑡) +𝑅𝑜𝑓𝑓 (𝑡 )

)

+2 𝐻 (𝑤− 𝐷) 1

𝑅𝑓𝑖𝑙

𝑀𝑒

𝑅

𝑂𝑓𝑓

𝑅

𝑢
(41)

• Memristance based on

• Due to the shape, varies with

M: TIME-DEPEDENDANT EXPRESSION FOR THE VOLUMES

𝑀𝑒

𝑅

𝑂𝑓𝑓
(42)

Vacancy Magnetic Field

G can be solved by

where we use and

Vacancy Magnetic Field

𝑀𝑒

𝑅

𝑂𝑓𝑓

𝑅

𝑢
(43)
(44)

is the surface normal for area infinitesimal

Wb

For Strukov’s device: b [1]

As [2]

, and

MEMORY FUNCTION

(45)

Not as easy as it looks.

(46)

𝑅

𝑓𝑖𝑙

=

𝑟

1

𝐷

𝑓

+

1

FILAMENT RESISTANCE

𝑀𝑒

𝑅

𝑂𝑓𝑓

𝑅

𝑢
(47)

EQUIVALENT CIRCUIT DIAGRAM TO THE DEVICE

CHEMISTRY

𝑅𝑇𝑜𝑡(𝑡)= 1

1

(

𝑅𝑢+𝑀𝑒(𝑡) +𝑅𝑜𝑓𝑓 (𝑡 )

)

+2 𝐻 (𝑤− 𝐷) 1

𝑅𝑓𝑖𝑙

𝑀𝑒

𝑅

𝑂𝑓𝑓

𝑅

𝑢
(48)

Experiment Theoretical Model

(49)
(50)

• Memristance is a phenomenon associated with ionic current flow

• Therefore  calculate the magnetic flux of the IONS

Vacancy Volume Current  , L = eLectric field

Vacancy Magnetic Field

Vacancy Magnetic Flux

Starting From The Ions…

(51)

Vacancy Volume Current

,

L = eLectric field

Calculate the Magnetic B

field Associated with the

ions

𝑀𝑒

𝑅

𝑂𝑓𝑓
(52)

• Memristance is a phenomenon associated with ionic current flow

• Therefore  calculate the magnetic flux of the IONS

Vacancy Volume Current  , L = eLectric field

Vacancy Magnetic Field

Vacancy Magnetic Flux

Starting From The Ions…

(53)

• Filamentary addition to the Mem-Con model gives

good qualitative

agreement to experiment

Work out the quantitative values

Re-do derrivation allowing a back-ground bulk

memristance

Conclusions Further Work

(54)

Ben de Lacy Costello

Andrew Adamatzky

David Howard

Larry Bull

With Thanks to

Steve Kitson (HP

UK)

David Pearson (HP

UK)

Bristol Robotics

(55)
(56)

• A larger study to test Georgiou et al’s model has been undertaken

• Repetition of size experiments with a different memristor at a different lab

(57)
(58)

Influx of Ionic I Voltage Spike Axon: Transmission along neuron Synapse: Transmission between neurons

(59)

Memristive Systems to

Describe Nerve Axon

(60)
(61)

• Memristance is a phenomenon associated with ionic current flow

• Therefore  calculate the magnetic flux of the IONS

Vacancy Volume Current  , L = eLectric field

Vacancy Magnetic Field

Vacancy Magnetic Flux

Starting From The Ions…

(62)

• Definition based on behaviour

• UPS – Voltage polarity irrelevant

• BPS –Voltage polarity relevant

• Pinched hysteresis loop in I-V space

• Different behaviour based on forming process,

complience current

• Satisfy Chua’s definition:

• Pinched hysteresis loop in I-V space

--ReRAM Memristor

(63)

The Memristor as a Synapse

Before learning Before learning

During learning

(64)

Process by which synapses are

potentiated

Related to Hebb’s Rule

Possibly a cause of memory and learning

Relative timing of spike inputs to a

synapse important

Spike-Time Dependent

Plasticity, STDP

Bi and Poo, Synaptic Modifications in Cultured Hippocampal Neurons:

(65)
(66)
(67)

Charge-Controlled

Memristor

Flux-Controlled

Memristor

Chua’s Definitions of Types of

Memristors

(68)

φ

q

V

I

(69)

What the Flux?

𝑑 𝜑

=

𝑀

(

𝑞

(

𝑡

)

)

𝑑𝑞

𝑀

(

𝑞

(

𝑡

)

)

=

𝑅

𝑜𝑓𝑓

𝜇

𝑣

𝐷

2

𝑅

𝑜𝑓𝑓

𝑅

𝑜𝑛

𝑞

(

𝑡

)

But, where is the magnetic flux?

𝑉

=

𝑀

(

𝑡

)

𝐼

(70)

• Memristance is a phenomenon associated with ionic current flow

• Therefore  calculate the magnetic flux of the IONS

Vacancy Volume Current  , L = eLectric field

Vacancy Magnetic Field

Vacancy Magnetic Flux

(71)

Mem-Con Theory

𝑞

𝑀(𝑞 )

𝜑

𝑉

𝑅

𝑡𝑜𝑡

(𝑡)

𝐼

Ionic

Electronic

(72)

Pictures

Curved (BPS -like) Memristors

Triangular (UPS -like) Memristors

(73)
(74)

To make a

memristor brain

& thus a machine

intelligence

(75)
(76)

Connecting Memristors with Spiking

Neurons to Implement STDP

1. Zamarreno-Ramos et al, On Spike Time Dependent Plasticity, Memristive Devices and Building a Self-Learning Visual Cortex, Frontiers in Neuroscience, 2011

0. Linares-Barranco and Serrano-Gotarredona, Memristance can

explain Spike-Time-Dependent-Plasticity in Neural Synapses, Nature Preceedings, 2009

(77)

Memristors

Spike

Naturally!

(78)
(79)

Voltage Square Wave

Current Spike Response
(80)

Voltage Ramp

Current Response

(81)

Neuro n

Memrist or

Memristor Behaviour Looks

Similar to Neurons

(82)
(83)

Pershin and Di Ventra, Spin Memristive Systems: Spin Memory Effects in Semi-conductor Spintronics, Phys. Rev. B, 2008

(84)
(85)

Direction of Spikes is related to not

V

The switch to 0V has a associated

current spike

Spikes are repeatable

Spikes are reproducable

Spikes are seen in bipolar switching

memristors/ReRAM

Spikes are not seen in unipolar

switching, UPS ReRAM type

memristors

(86)

Curved (BPS -like)

Memristors

Triangular (UPS

-like) Memristors

(87)

Where do the Spikes

Come From?

(88)

q

φ

I

V

q

φ

V

I

Neurons

Memristors

Mem-Con Model Applied to

(89)

Dynamics related to min.

response time, τ, related to speed of ion diffusion across membrane

Memory property = ???Neuron operated in a

current-controlled way

Dynamics related to

τ, which is related to

Memory property =

q

v

Memristor operated

in voltage controlled

way

Neuron Voltage Spikes

Memristor Current

Spikes

(90)

More complex system than a single

memristor

Short-term memory associated with

membrane potential

Long term memory associated with

the number of synaptic buds

(91)

Sol-Gel Memristor

Negative V

Sol-Gel Memristor

Positive V

(92)
(93)
(94)
(95)
(96)

I-t Response to

Stepped Voltage

Time Dependent

I-V

(97)

Voltage Ramp

Current Response

(98)
(99)

Neurology:

Modelling Neurons with the Mem-Con

Theory to prove that they are Memristive

Investigate the Memory Property for

neurons

Unconventional Computing:

Further Investigation of memristor and

ReRAM properties

Attempt to build a neuromorphic control

system for a navigation robot

(100)
(101)

Neurons May Be Biological Memristors

Neurons Operate via Voltage Spikes

Memristors can Operative via Current

Spikes

Thus, Memristors are Good Candidates for

Neuromorphic Computation

A Memristor-based Neuromorphic

Computer will be Voltage Controlled and

transmit data via Current Spikes

(102)

References

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