26
1 CHEM.4008/4061. 2004/2005. Electroactive Nanostructured Materials. Dr Mike Lyons Chemistry Department Room 2.02 SNIAM. Email: [email protected] Electroactive Nanostructured Materials. Lecture 1/2.

Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

  • Upload
    others

  • View
    1

  • Download
    0

Embed Size (px)

Citation preview

Page 1: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

1

CHEM.4008/4061.2004/2005.Electroactive NanostructuredMaterials.

Dr Mike LyonsChemistry Department

Room 2.02 SNIAM.Email: [email protected]

Electroactive NanostructuredMaterials.

Lecture 1/2.

Page 2: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

2

Course Summary.• 4/6 lectures. 4 lectures for SS Chemists, 6 lectures for SS

Advanced Materials. These will will mainly cover:

– Introduction to electroactive nanostructured materials.– Self assembled electroactive monolayers and monolayer protected

clusters (MPC’s).– Electronically conducting polymer materials.– Redox polymer materials.– Catalysis/sensing using electroactive polymer thin films.– Transport and kinetics within electroactive polymer thin films :

theory and experiment.

• Main reference : Electroactive polymer electrochemistry (Lyons), Plenum Press, 1994/1996, available in Hamilton Library.Also some review articles which will be given out during course.

ElectroactiveNanostructured Materials

Motivations/Introduction.

Page 3: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

3

Electroactive nanostructuredmaterials.

• Electroactive materials can be assembled on the surface of a support electrode to form a ‘tailormade’ or chemically modified electrode (CME).

• The electrode surface may be modified either with an ordered monolayer film or a multilayer polymer film.

• These materials exhibit a capacity to:– Pass electric current.– Store charge.– Display redox activity.

• Sites in monolayer/polymer film may undergo oxidation/reduction when a potential is applied to the material.

• Applications:– Battery materials– Electrochromic displays– Microelectronic devices– Molecular electronics– Electrocatalysis– Chemical/biological sensor technology– Energy conversion– Corrosion protection– Actuators.

Chemically Modified Electrodes.

Page 4: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

4

Nanoscience and Nanotechnology.

Page 5: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

5

Small is beautiful !Molecular Electronics.

Molecular Electronics/ICT

Page 6: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

6

Page 7: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

7

ElectronicsReceptor

TransducerSubstrate(analyte)

Interferentspecific molecular recognitionbetween substrate and receptor site

chemical interactiontranslated into a usefulsignal

data transformedand processedinto usefulformat

Chemical/BiologicalSensor Configuration.

A biosensor is a device that recognizes an analyte in an appropriate sample and interprets its concentration as an electrical signal via a suitable combination of a biological recognition system and a suitable transducer.

Mediated Electron Transfer

Page 8: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

8

Enzyme communication with electrodes.

Page 9: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

9

Amperometric enzyme biosensor for glucosemeasurement.

Enzyme biosensor: uses electron transfer mediatorin electrochemical detection step.

Page 10: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

10

Self Assembled Monolayers(SAM)

Fundamental Properties.

Chemically modified electrodes:2D vs 3D nanostructures.

• Monolayer derivitized electrodes developed first.• New interest in these systems:

– Redox active self assembled monolayers. e.g. ferrocenecontaining alkane thiols.

• CME systems based on 3D microstructures. E.g. electroactive polymer thin films such as poly(vinylferrocene), poly(pyrrole).

• These materials are preferable for chemical sensor and electrocatalytic systems, since there is a 3D dispersion of active sites throughout the material and a high concentration of active sites is achieved even though the quantity of active material is small.

Page 11: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

11

Monolayer vs multilayer modified electrodes.

3D nanostructure.Redox active multilayer.Surface coverage ca. 10-8 molcm-2

2D nanostructure.Redox active monolayer.Surface coverage ca. 10-10 mol cm-2.

Redox active sites

Alkanethiol SAM’s:Ordered nano-assemblies.

• The formation of organized monolayers at metallic surfaces through self assembly provides an attractive method for the preparation of nanostructured ensembles with well defined composition, structure and thickness.

• These self assembled monolayers (SAM) have been used as model systems to test modern theories of interfacial electron transfer dynamics across organic spacers in a controlled manner.

• Redox active SAM ensembles, consisting of ferrocene units covalently attached to alkane thiol connectors adsorbed on gold substrate surfaces, especially when mixed and diluted with non-electroactive alkanethiols, also serve as good mechanically robust models for molecular wires and individual molecular nanoelectrodesystems.

Page 12: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

12

Page 13: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

13

Alkane thiol SAM formation.

Oxidative addition ofSH bond to Au surfacefollowed by reductiveelimination of hydrogen.

Alkanethiol SAM Formation

Page 14: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

14

Alkanethiol Self Assembly Mechanism

SAM Formation : Adsorption kinetics.Adsorption usually occurs on a far shorter timescale (minutes) than self Assembly (hours, days).We model the adsorption process via a Langmuir Isotherm.Controversy exists regarding the exact nature (electrochemical vsnon-electrochemical) of the adsorption mechanism.

221 HMRSHRSM +−→−+ −+ ++−→+− eHMRSMHRS

Traditional non EC mechanism New EC mechanism

Adsorption process examined usually via optical (Second Harmonic Generation SHG) or gravimetric (electrochemical quartz crystal microbalanceEQCM) techniques.Adsorption occurs mainly by dipping metal support into solution containingalkane thiol at low concentration (0.1 µM-1 mM) either at open circuit but alsowhen the metal is subjected to an applied potential (typically 0.2-0.6 V).Monolayer film formed under potential control exhibits better packing and orderand forms much more rapidly.

Page 15: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

15

EQCM Fundamentals.• The quartz crystal microbalance (QCM) is a variant of acoustic wave

microsenseors that are capable of ultrasensitive mass measurements. Under favorable conditions, a typical QCM can measure a mass change of 0.1-1 ng/cm2.

• The QCM oscillates in a mechanically resonant shear mode (determined by the dimensions of the crystal and the mass loading) under the influence of a high frequency AC electric field which is applied across the thickness of the crystal. A change in the mass of the working electrode causes a change in the resonant frequency of the piezoelectric device, which can then be related directly to the quantity of added mass via the Sauerbrey equation:

where Cf is a constant which depends on the density ρ of the crystal, µ the shear modulus of quartz , the area A of the gold coated quartz disc , and f0the resonant frequency of the fundamental mode of the crystal.

• Hence an increase in mass implies a decrease in frequency and one can use small changes in frequency to monitor very small changes in mass in a very accurate manner.

mCf f ∆−=∆A

fC f ρµ

202

=

Electrochemical Quartz Crystal Microbalance.

Sauerbrey Equation

f = [-2f02 / A(mr)1/2] m

For:

f = 1Hz

fi m = 1.4ng

↑∆↓∆

=

∆−=∆−=∆

masf

fC

QnFMmCf

f

f

20

2ρµ

Page 16: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

16

EQCM: thiol adsorptionLee et al. Bull. Kor. Chem. Soc. 2001,22,276

Langmuir Adsorption Isotherm

( ) θθθDA kck

dtd

−−= 1Σ

=ΓΓ

=NNU

m

θVU NNN +=Σ

SAM coverage expressed in terms of the fractional surface coverage θ with0≤θ≤1. The latter quantity represents the fraction of available siteswhich have reacted.

# vacant sites

# occupied sites

Total # sites

Γ= surface coverage (typically nmol/cm2 range)Γm = monolayer surface coverage

Net rate of adsorption

Adsorption rateConstant M-1s-1

Desorption rateConstant s-1

Integrate rate eqn. using initial condition : θ = 0, t = 0

( ) ( )[ ]{ }tkckkkc

ct DAAD

+−−+

= exp1θ

[ ]( )tkt obs−−= exp1)( κθ

A

D

kkc

c

+=κ

DAobs kckk += Intercept = kD

Slope =kA

kobs

c

Adsorbate concentration

Diagnostic Plot

Page 17: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

17

Equilibrium constant K (M-1)

D

A

kkK =

Steady state fractional coverage θ(∞)occurs when t ∞

( )KcKc+

=∞1

θ

KRTGads ln−=∆

Gibbs energy of adsorption

Langmuir Model provides convenientfirst approach to extract quantitativekinetic and thermodynamic data forthiol adsorption from solution.

Page 18: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

18

Self Assembly Kinetics

Fit to Langmuir Adsorption Isotherm.

Optical monitoring of adsorption/Self assmbly

SAM surface structure• STM & AFM very useful

to obtain surface topography of alkanethiol SAMs.

• 2 types of coexisting molecular lattices observed for SAMs on Au(111) surfaces– (√3x√3 )R30°structure– C(4x2) superstructure

Page 19: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

19

Page 20: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

20

Modified Randles Equivalent Circuit Model : SAM coated metal

SAMDL

SAMD

DSAMDL

CCCC

CCC

≅>>

+=111

LC rSAM

εε0=

L

5≅rε

CE

RE

WE

RF

RCT ZW

RS

CDL

Thiol film capacitanceCSAM inversely proportional to monolayer thickness L.

Layer thickness Lproportional tothiol chain length n.

Alkane thiol filmmodelled as simpleparallel platecapacitor.

SAM Quality Control: Blocking solution phase interfacial ET reactions

Poor monolayer: pinholes present.

0 200 400 600 800 1000 1200-1.5e-5

-1.0e-5

-5.0e-6

0.0

5.0e-6

1.0e-5

1.5e-5

I p/A

E/mV

0 200 400 600 800 1000 1200-1.5e-5

-1.0e-5

-5.0e-6

0.0

5.0e-6

1.0e-5

1.5e-5

I p/A

E/mV

Bare gold

SAM/Au

Bare gold

SAM/Au

0 200 400 600 800 1000 1200-1.5e-5

-1.0e-5

-5.0e-6

0.0

5.0e-6

1.0e-5

1.5e-5

I p/A

E/mV

0 200 400 600 800 1000 1200-1.5e-5

-1.0e-5

-5.0e-6

0.0

5.0e-6

1.0e-5

1.5e-5

I p/A

E/mV

Bare gold

SAM/Au

Bare gold

SAM/Au

))(()(// 3/46 aqKClCNFeSAMAu −−

))(()(/ 3/46 aqKClCNFeAu −−

Good monolayer: redox activity of solution phaseredox couple at underlying gold electrodeblocked.

• Non redox active C12 alkanethiol monolayer generated via immersing gold substrate electrodes in 1mM dodecanethiol in EtOHsolution for 48hrs. • Integrity of monolayer formed via self assembly checked by immersion of electrode in 2mM Ferrocyanide/Ferricyanide solution in 1M KClsolution for 24 hrs and recording the resultant cyclic voltammogram. • Ferrocyanide/ferricyanide redox behaviour well defined at bare gold electrode. In absence of pinholes in monolayer film no trace of ferrocyanide/ferricyanide redox activity should be observed since the ET kinetics of the solution phase redox couple will be effectively blocked because of greatly reduced electronic coupling between redox couple and Au electrode.

Page 21: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

21

Redox active monolayers : alkanethiol self-assembled monolayers (SAM).

• Alkane thiol monolayer generated either via LB method or by self assembly.

• Both electroactive, non-electroactive, and‘mixed’ SAM systems readily generated.

• Wide range of redox groups can be attached to alkane chain : ferrocenes, quinones, azobenzenes, viologens, cytochrome c etc.

• Can readily achieve dilution of electroactive component in a mixed monolayer.

• Applications: – Microarray electrodes – Selective permeation– Pre-concentration & selective

binding– Electrocatalysis– Long range ET– Corrosion and adhesion control.

~ 300

Co-adsorption of ferrocene-terminatedalkane thiol and an unsubstituted alkanethiol on Au(111).

~ 20 Å

Redox labeled alkane thiols : Synthetic Strategy.

ClO

FeFe

ClO

Cl+AlCl3

CH2Cl2

0 - 25°C

ClO

FeOH

O

Fe

Red Solid,

94 – 96%

Step 1: Synthesis of (2-Chlorobenzoyl)Ferrocene•Friedel-Crafts Acylation

•Ketone product is weakly basic forming a catalytically inactive complex with the Lewis acid (AlCl3)

•Ketone product is isolated by destroying the complex using ice-water

Step 2: Synthesis of Ferrocene Carboxylic Acid•Cleavage of benzyl chloride by OH- ion

•10:3 ratio of t-BuOK to water

Yellow Solid,

74 – 83%H2O, t-BuOK, ∆

DME

ClO

FeFe

ClO

Cl+AlCl3

CH2Cl2

0 - 25°C

ClO

FeOH

O

Fe

Red Solid,

94 – 96%

Step 1: Synthesis of (2-Chlorobenzoyl)Ferrocene•Friedel-Crafts Acylation

•Ketone product is weakly basic forming a catalytically inactive complex with the Lewis acid (AlCl3)

•Ketone product is isolated by destroying the complex using ice-water

Step 2: Synthesis of Ferrocene Carboxylic Acid•Cleavage of benzyl chloride by OH- ion

•10:3 ratio of t-BuOK to water

Yellow Solid,

74 – 83%H2O, t-BuOK, ∆

DME

Step 3: Synthesis of n-(Ferrocenylcarbonyloxy)(CH2)n Bromide•Mitsunobu Coupling Reaction

•DMAP added in catalytic amounts of 3-10%

O

O

Brn

Fe

OH Brn OH

O

Fe+ DCC, DMAP

CH2Cl20 - 25°C

Brown Solid

74% Yield

Step 4: Synthesis of n-(Ferrocenylcarbonyloxy)(CH2)n Thiol•Iso-thiuronium salt produced by EtOH reflux

•Iso-thiuronium salt is cleaved by an OH- ion in the KOH reflux

•The nucleophilic RS- is then washed with dilute HCl giving the thiol group (RSH)

EtOH (100%), ∆ (24hrs) O

O

SHn

FeNH2 NH2

SO

O

Brn

Fe+

KOH (aq), ∆ (4hrs)Brown Solid

53% Yield

Step 3: Synthesis of n-(Ferrocenylcarbonyloxy)(CH2)n Bromide•Mitsunobu Coupling Reaction

•DMAP added in catalytic amounts of 3-10%

O

O

Brn

Fe

OH Brn OH

O

Fe+ DCC, DMAP

CH2Cl20 - 25°C

Brown Solid

74% Yield

Step 4: Synthesis of n-(Ferrocenylcarbonyloxy)(CH2)n Thiol•Iso-thiuronium salt produced by EtOH reflux

•Iso-thiuronium salt is cleaved by an OH- ion in the KOH reflux

•The nucleophilic RS- is then washed with dilute HCl giving the thiol group (RSH)

EtOH (100%), ∆ (24hrs) O

O

SHn

FeNH2 NH2

SO

O

Brn

Fe+

KOH (aq), ∆ (4hrs)Brown Solid

53% Yield

• Method suitable for preparation of C5 – C12 alkane thiols.

• C5 – C12 bromo-alcohols available commercially.

Page 22: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

22

Redox switching in alkane thiol SAM’s.

−+−+

−+

−→+−

+−→−

XFcRXFcReFcRFcR

• Oxidative redox switching involves both a redoxtransformation Fc Fc+

(oxidation state change) and a coupled ion transfer/binding process to form ion pair Fc+X-. Reverse sequence occurs on reductive switching step.

• Can label reaction sequence as an EC process (E – redox ET, C –ion pair formation).

• ET chemistry and dynamics examined via cyclic voltammetry(CV).

• Ion pairing/transport examined via Electrochemical Quartz Crystal Microbalance (EQCM).

Potential (V)

0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9

Cur

rent

(A)

-8e-6

-6e-6

-4e-6

-2e-6

0

2e-6

4e-6

6e-6

8e-6

Typical CV profile (0.1 M HClO4 ) of Ferrocenebased electroactive alkanethiol monolayer film.

S(CH2)10CO2 Fc = R-Fc

R-Fc R-Fc+

R-Fc+ R-Fc

Page 23: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

23

Cyclic Voltammetry study of ferrocene based electroactivethiols of varying alkane chain length.

7Fc thiol

Potential (V)0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9

Cur

rent

(A)

-3e-6

-2e-6

-1e-6

0

1e-6

2e-6

3e-6

4e-6 8Fc thiol

Potential (V)0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9

Cur

rent

(A)

-4e-6

-2e-6

0

2e-6

4e-6

6e-6

10Fc thiol

Potential (V)0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9

Cur

rent

(A)

-8e-6

-6e-6

-4e-6

-2e-6

0

2e-6

4e-6

6e-6

8e-6 12Fc thiol

Potential (V)0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9

Cur

rent

(A)

-1e-5

-8e-6

-6e-6

-4e-6

-2e-6

0

2e-6

4e-6

6e-6

8e-6

1e-5

18.0858257858612

15.0557357057510

17.785645605688

35.965655625687

FWHM(mV)

∆E(mV)

E0

(mV)EPC

(mV)EPA

(mV)

AlkaneChain Length

CV parameters for CV parameters for ferroceneferrocene containing containing electroactiveelectroactive thiolsthiols ((CCnn--FcFc--SAMSAM).).

6.112

5.510

3.38

0.66

1010Γ/mol cm-2n

Page 24: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

24

Potential (V)0.3 0.4 0.5 0.6 0.7 0.8

Freq

uenc

y (H

z)

-60

-50

-40

-30

-20

-10

0

10

Cur

rent

(A)

-4e-5

-3e-5

-2e-5

-1e-5

0

1e-5

2e-5

3e-5

4e-5

EQCM study of EQCM study of redoxredox switching in switching in ferroceneferrocene based SAM based SAM films. films.

Sauerbrey Equation

f = [-2f02 / A(mr)1/2] m

For:

f = 18.5Hz

fi m = 2.59 x 10-8 g

This is approximately equivalent to one perchlorateion per redox site being incorporated onto the SAM surface

Potential (V)0.0 0.2 0.4 0.6 0.8 1.0

Del

ta F

requ

ency

(Hz)

-25

-20

-15

-10

-5

0

Cur

rent

(A)

-4e-6

-2e-6

0

2e-6

4e-6

12 Fc thiol. CV + EQCM

10 Fc thiol. CV + EQCM

11 Fc thiol. CV + EQCM11Fc thiol. CV + EQCM

Potential (V)

0.3 0.4 0.5 0.6 0.7 0.8

Freq

uenc

y (H

z)

-20

-15

-10

-5

0

5

Cur

rent

(A)

-5e-6

0

5e-6

1e-5

EQCM study of redox behaviour of ferrocenebased electroactive thiols

2.55 x 10-8-18.28

2.59 x 10-8

2.70 x 10-8

Mass Change(g)

-18.5

-19.6

Frequency Change

(Hz)

12

7

Alkane Chain Length

(S(CH2)nCO2Fc )

Page 25: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

25

Laviron Model : LPS Voltammetry

• Assume oxidative surface redoxreaction.

• Neglect interaction effects between surface immobilized groups.

• Develop normalisedLPSV response of Ψ = Ψ(ξ).

( )0

2

EERTF

RTAFi

−=

Γ=Ψ

Σ

ξ

υ

[ ][ ]( ) ( )

−=Ψ

+=

−+−

=Ψ−

ββ ηβ

η

ηη

ξξ

mm exp

1exp1exp

EIrrev

21

1

2ERev

[ ]

RTFkkm

υσ

ξη00

exp

==

=

E. Laviron J. Electroanal. Chem. 101 (1979) 19-28.

Theoretical LPS voltammograms:Surface redox reaction.

ξ = F(E-E0)/RT

-10 -8 -6 -4 -2 0 2 4 6 8 10

Ψ =

i/(F

2 AΓ Σ

ν /R

T)

0.00

0.05

0.10

0.15

0.20

0.25

0.30

Esurf(Rev)Esurf(Irrev)

Page 26: Electroactive Nanostructured Materials. 2005 L1-2.pdf · Advanced Materials. These will will mainly cover: – Introduction to electroactive nanostructured materials. – Self assembled

26

Potential Step Chronoamperometry: Quantifying

Surface ET Dynamics

• Potential Step Chronoamperometry can be used to probe the dynamics of a fast surface electron transfer reaction within a monolayer film.

• Apply large amplitude potential step and monitor resulting current variation (arising from surface ET event) as a function of time.

• Ideally first order kineticsexhibited by surface ET process.

0 2 4 6 8 10-4.4-4.2-4.0-3.8-3.6-3.4-3.2-3.0-2.8-2.6-2.4-2.2

t / ms

Log(

i/A)

Oxidation Transient

Reduction Transient

( ) [ ]

( )

−=

Γ=∆−∆=

Σ

RTEEF

kk

nFAQtkQkti

BAETET

ETET

0,0 exp

exp

β

PS amplitude: 400 mV From 440 880 mV (oxidation)And 880 440 mV (reduction)10 ms pulse width. C12-Fc-thiol

redox activegroup A/B

alkane chain

gold electrode

kET

redox activegroup A/B

alkane chain

gold electrode

kET

Charge passed during transient

ET rate constantdepends on potential ( )

( ) 1

1

2.53.67reduction

5.11.24oxidation−

±=

±=

sk

sk

ET

ET

PS chronoamperometry: Fc labelledC12- alkanethiol SAM film.

• PS chronoamperometric transients recorded in 1st order semi-logarithmic format for the C12 Fc-alkanethiol monolayer.

• Transient current response corresponds to electron tunneling through hydrocarbon chain brought about by the potential step induced surface bound ferrocene/ferricinium redoxtransition.

• Current Decay kinetics more rapid in the presence (black curve) of an external magnetic field of magnitude 0.5 T than in the absence (red curve) of the field .

• Potential step 300 - 850 mV (oxidation) and 850-300 mV (rediction). Timescale 10 ms. Supporting electrolyte: 0.1M HClO4.

B = 0.5 T

B = 0 T

B = 0 T

B = 0.5 T

oxidation

reduction