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Electrochemistry in Nanoelectronics & Nanosensors N.J. Tao N.J. Tao Arizona State University Arizona State University

Electrochemistry in Nanoelectronics & Nanosensors

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Electrochemistry in Nanoelectronics & Nanosensors. N.J. Tao Arizona State University. Next: Google Nano?. Google Earth Google Sky. NANO-Building Blocks. Resonator. Particle. Rod. Peptide Tube. “Nano”. Carbon Tube. Belt. Wire. Pyramid. This lecture. Electrochemistry. - PowerPoint PPT Presentation

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Page 1: Electrochemistry  in Nanoelectronics & Nanosensors

Electrochemistry in Nanoelectronics & Nanosensors

N.J. TaoN.J. Tao

Arizona State UniversityArizona State University

Page 2: Electrochemistry  in Nanoelectronics & Nanosensors

Next: Google Nano?Next: Google Nano?

Google EarthGoogle EarthGoogle SkyGoogle Sky

Page 3: Electrochemistry  in Nanoelectronics & Nanosensors

“Nano”

Rod

Carbon Tube

WireBelt

ParticleResonator

Peptide Tube

NANO-Building Blocks

Pyramid

Page 4: Electrochemistry  in Nanoelectronics & Nanosensors

Electrochemistry

NanoelectronicsNanosensors

This lecture

Page 5: Electrochemistry  in Nanoelectronics & Nanosensors

Electrochemical NanofabricationElectrochemical Nanofabrication

• Electrodeposition & etchingElectrodeposition & etching

Page 6: Electrochemistry  in Nanoelectronics & Nanosensors

Electrodeposition: Electrodeposition: Then … andThen … and Now…Now…

• Ancient origin. Romans soldered silver plates to articles of metals and in the 5th century iron weapons were coated with copper by dipping them in a copper solution. During the 18th century, plating of copper or brass with silver by fusion started in England.

• IBM announced in1997 a new advance in semiconductor process that entails replacing aluminum with copper. Cu has less "resistance" than Al.

Page 7: Electrochemistry  in Nanoelectronics & Nanosensors

Local Probe Approach (STM & AFM)

The clusters can be dissolved by changing the sample potential and afterwards the blank Au surface can be imaged again.

Array of 10 x 10 Cu clusters at Esubstrate = +10 mV vs. Cu/Cu2+.

The same surface area after complete dissolution of the clusters at Esubstrate = +300 mV.

Kolb et al, 1998

Page 8: Electrochemistry  in Nanoelectronics & Nanosensors

Template Methods: Negative

Nanowires

• The beginning: Possion used etched ion tracks in mica sheets as templates to fabricate metal wires. P. E. Possion, Rev. Sci. Instrum. 41, 772 (1970).

• The templates: Ions tracks in mica or polycarbonate membranes, anodized alumina, phase segregated copolymer films are the popular choices.

Page 9: Electrochemistry  in Nanoelectronics & Nanosensors

Building Block of Nanoelectronic Devices – Molecular Junctions

Top: Scheme for preparing nanowire devices by:1)self-assembly of a MHDA monolayer, or 2)layer-by-layer assembly of TiO2 /PSS multilayer film on the exposed tip of a bottom metal electrode, followed by electroless seeding and electroplating of a top metal electrode.

Penn State Group

Page 10: Electrochemistry  in Nanoelectronics & Nanosensors

Building Block of Nanoelectronic Devices – CdSe Nanojunctions

Au-CdSe-Au

Ni-CdSe-Ni

Penn State Group. J. Phys. Chem. 106, 7458(2002)

• Graph of CdSe segment length vs the number of cyclic voltammetric scans for 350-nm diameter nanowires. Error bars show the standard deviation in length.

Page 11: Electrochemistry  in Nanoelectronics & Nanosensors

Positive Templates

• Positive template method uses wire-like nanostructures, such as DNA and carbon nanotubes, as templates, and nanowires are formed on the outer surface of the templates.

• Unlike negative templates, the diameters of the nanowires are not restricted by the template sizes and can be controlled by adjusting the amount of materials deposited on the templates.

Page 12: Electrochemistry  in Nanoelectronics & Nanosensors

AuPt

• After Pt or Au deposition on SWNTs, the sample was annealed at 600°C in air for 10 min, which leads to Pt/Au nanoparticles forming chain-like structures.• In contrast to ordinary electroless deposition, no reducing agents are needed for SWNTs.

Carbon Nanotube Template

Dai et al JACS 124(31)9058, 2002.

Page 13: Electrochemistry  in Nanoelectronics & Nanosensors

DNA Template

• The first step is to fix a DNA strand between two electrical contacts. • The DNA is then exposed to a solution containing Ag+ ions. The Ag+ ions bind to DNA and are then reduced by a basic hydroquinone solution to form Ag nanoparticles decorating along the DNA chain. • The nanoparticles are further ‘developed’ into a nanowire using a photographic enhancement technique.

Braun, E. et al. Nature 391, 775, 1998

Page 14: Electrochemistry  in Nanoelectronics & Nanosensors

Graphite Step Edge Template

Step 1: Electrodeposit Pd Step 1: Electrodeposit Pd nanowires.nanowires.

Step 2: Transfer the Pd wires to a Step 2: Transfer the Pd wires to a glass slide.glass slide.

Step 3: Apply silver contacts.Step 3: Apply silver contacts.

Step 1

Step 2

Step 3

Penner et al.

Page 15: Electrochemistry  in Nanoelectronics & Nanosensors

Graphite Step Edge Template

Penner et al.

Page 16: Electrochemistry  in Nanoelectronics & Nanosensors

ApplicationsApplications

• Nanoelectronics• Nanomechanics;• Optoelectronics;• Chemical and biosensors;• Catalysis;• Energy related;• - …..

Page 17: Electrochemistry  in Nanoelectronics & Nanosensors

Electrochemistry

NanoelectronicsNanosensors

Page 18: Electrochemistry  in Nanoelectronics & Nanosensors
Page 19: Electrochemistry  in Nanoelectronics & Nanosensors

When will computer hardware match the human brain?Hans Moravec

Robotics Institute Carnegie Mellon University

Pittsburgh, PA 15213-3890, USA

“The 100 million MIPS to match human brain power arrive in home computers before 2030”

MIPS – Million Instructions per Seconds

Page 20: Electrochemistry  in Nanoelectronics & Nanosensors

Nanoelectronics

Single Electron Transistor

• Electronics based on new phenomena occurring at Nano-scale

Molecular Electronics

Ballistic transport

Electron tunneling

Spintronics

Kondo effect

Localization

Page 21: Electrochemistry  in Nanoelectronics & Nanosensors

Single Electron Transistor (SET)

Page 22: Electrochemistry  in Nanoelectronics & Nanosensors

What is a transistor (FET)?

p+ orn+ Si

p+ orn+ Si

OXIDE LAYER

n- or p-TYPE Si

0 V

Vg0 V Vd > 0

GATEMETAL

Ec

EF

Ev

p-TYPE n-TYPEn-TYPE

Off (0)

Ec

EF

Ev

p-TYPE n-TYPEn-TYPE

On (1)

Gate

Source Drain

Page 23: Electrochemistry  in Nanoelectronics & Nanosensors

Single Electron Transistor

;2

2

C

eEeV

• Capacitor charging energy:

C

e

C

QE eQ

22

21

2

dC 02

TkC

eE B

2

2

• To avoid thermal broadening:

T=300 K (room temperature)

FC 1810

(a sphere)

sizeC ~Dot

Gate

Source Drain

EF

e2/C

Page 24: Electrochemistry  in Nanoelectronics & Nanosensors

What is Tunneling?

)(2

2EUm

LeT ~

Page 25: Electrochemistry  in Nanoelectronics & Nanosensors

Single Electron Transistor

Coulomb blockade

Coulomb staircase

• Charge is quantized• Electron Tunneling (R1, R2)

Dot

Gate

Source =

Page 26: Electrochemistry  in Nanoelectronics & Nanosensors

Local Oxidation with a Thin Water Film

STM or AFM tip

Water layer

Ti oxideTi film (3nm)Oxidation

• Substrate Electrode:

nenHMOOnHM n 222

• Tip Electrode:

nOHnHOnHne 222 22

• The thin water film is extremely important in the practical resolution of the fabricated structure. A controlled humidity is recommended.

Snow et al. Science, 270, 1639-41 (1995).

K. Matsumoto, Physica-B 227, 92-4 (1996).

100 nm

5 V

Page 27: Electrochemistry  in Nanoelectronics & Nanosensors

K. Matsumoto et al.~ 30 nm metal quantum dot

The island may seem to be big, but C, determined by the junction cross sectional area, is < 10-19F.

Room Temperature Single Electron Transistor

Page 29: Electrochemistry  in Nanoelectronics & Nanosensors

Conductance Quantization

Page 30: Electrochemistry  in Nanoelectronics & Nanosensors

L >> electron mean free pathD>> F, electron wavelength

L

2/ 2D

LR

2~1

DR

G

G changes continuously as D.

D

Conductance

D

G (G

0)

Classical conductance:

Page 31: Electrochemistry  in Nanoelectronics & Nanosensors

L < electron mean free path ballistic transport (no collisions).D~ F, electron wavelength wave nature of electron important.

D=FD=F/2

Motion

Free

Qua

n tiz

ed

N=1

Motion

Free

Qua

n tiz

ed

N=2

01

0 NGTGGN

nn

where, N=0, 1, 2, 3, …and G0 = 2e2/h=77S G

(G0)

D

12

3

4

5 F ~ 1-3 Å

Conductance Quantization

R0=13 k

Page 32: Electrochemistry  in Nanoelectronics & Nanosensors

Quantum Confinement & Standing Waves

Page 33: Electrochemistry  in Nanoelectronics & Nanosensors

Conductance Quantization Metal Nanowires

F ~ 1-3 Å – must be atomically thin! l e ~ nm.

Room temperature.

How to fabricate such wires?How to fabricate such wires?

Page 34: Electrochemistry  in Nanoelectronics & Nanosensors

substrate

RE

CE

Bipo

tentio

stat

Electrolyte

Metal wire

Substrate

insulation

Etching Deposition

tip

+ +

+

++

----

--

- --

+ +

+

++

+++

++

Electrochemical Fabrication

Li & TaoAppl. Phys. Lett.

Page 35: Electrochemistry  in Nanoelectronics & Nanosensors

0 1000 2000 3000 4000 5000 6000

Tim e (m s)

Co

ndu

ctan

ce (

2e2

/h)

Etching (dissolution)

2

4

6

8

10

Etching

0 20 40 60 80 100 120 140 160

Tim e (m s)

Co

ndu

ctan

ce (

2e2

/h)

Deposition

2

4

6

8

10

Deposition

Page 36: Electrochemistry  in Nanoelectronics & Nanosensors

From Conductance Quantization to Quantum Tunneling

or

Large gap

DepositionDeposition

EtchingEtching

Li & Tao, Nanotechnology, 10, 221(1999).Morpurgo et al., Appl. Phys. Lett., 13, 2082(1999).

Page 37: Electrochemistry  in Nanoelectronics & Nanosensors

Large gap

EtchingEtching DepositionDeposition

9.5

8.5

7.5

6.5

5.5

4.5

T im e (sec./d iv is ion)

0

1

2

3

-1

-2

Ga

p W

i dth

(A

)

l n (

I/nA

) Tunnelingcurrent

Ln(I) ~ width

Tunneling!

From Conductance Quantization to From Conductance Quantization to Quantum TunnelingQuantum Tunneling

Page 38: Electrochemistry  in Nanoelectronics & Nanosensors

-1

0

1

2

3

-2

-1

0

1

2

Ga

p W

idth

(A

)

7.5

8.5

9.5

8.5

6.5

5.5

7.5

6.5

5.5

4.5

ln (

I/ nA

)

10ms

a

b

I ~ exp(-bL) ln(I) ~ - LI ~ exp(-bL) ln(I) ~ - L

• StepwiseStepwise ln(I) ln(I) leads to leads to discrete change of discrete change of ss!!

Stepwise Tunneling Current – Log scale

s

• Discrete Nature of AtomDiscrete Nature of Atom