soft matter films interfaced to electronic devices

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Engineering Conferences International ECI Digital Archives Colloidal, Macromolecular & Biological Gels: Formulation, Properties & Applications Proceedings 7-13-2016 Soſt maer films interfaced to electronic devices: capacitance-modulated field effect transistors integrating protein layers Gerardo Palazzo Dept. of Chemistry and CSGI, University of Bari, Italy, [email protected] Luisa Torsi Dept. of Chemistry and CSGI, University of Bari, Italy Maria Magliulo Dept. of Chemistry and CSGI, University of Bari, Italy Antonia Mallardi CNR-IPCF, Bari, Italy Follow this and additional works at: hp://dc.engconfintl.org/cmb_gels Part of the Engineering Commons is Abstract and Presentation is brought to you for free and open access by the Proceedings at ECI Digital Archives. It has been accepted for inclusion in Colloidal, Macromolecular & Biological Gels: Formulation, Properties & Applications by an authorized administrator of ECI Digital Archives. For more information, please contact [email protected]. Recommended Citation Gerardo Palazzo, Luisa Torsi, Maria Magliulo, and Antonia Mallardi, "Soſt maer films interfaced to electronic devices: capacitance- modulated field effect transistors integrating protein layers" in "Colloidal, Macromolecular & Biological Gels: Formulation, Properties & Applications", ECI Symposium Series, (2016). hp://dc.engconfintl.org/cmb_gels/29

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Engineering Conferences InternationalECI Digital ArchivesColloidal, Macromolecular & Biological Gels:Formulation, Properties & Applications Proceedings

7-13-2016

Soft matter films interfaced to electronic devices:capacitance-modulated field effect transistorsintegrating protein layersGerardo PalazzoDept. of Chemistry and CSGI, University of Bari, Italy, [email protected]

Luisa TorsiDept. of Chemistry and CSGI, University of Bari, Italy

Maria MagliuloDept. of Chemistry and CSGI, University of Bari, Italy

Antonia MallardiCNR-IPCF, Bari, Italy

Follow this and additional works at: http://dc.engconfintl.org/cmb_gels

Part of the Engineering Commons

This Abstract and Presentation is brought to you for free and open access by the Proceedings at ECI Digital Archives. It has been accepted for inclusionin Colloidal, Macromolecular & Biological Gels: Formulation, Properties & Applications by an authorized administrator of ECI Digital Archives. Formore information, please contact [email protected].

Recommended CitationGerardo Palazzo, Luisa Torsi, Maria Magliulo, and Antonia Mallardi, "Soft matter films interfaced to electronic devices: capacitance-modulated field effect transistors integrating protein layers" in "Colloidal, Macromolecular & Biological Gels: Formulation, Properties& Applications", ECI Symposium Series, (2016). http://dc.engconfintl.org/cmb_gels/29

SOFT MATTER FILMS INTERFACED TO ELECTRONIC

DEVICES: CAPACITANCE-MODULATED FIELD EFFECT

TRANSISTORS INTEGRATING PROTEIN LAYERS

Gerardo Palazzo1,2, Mulla Yusuf Mulla1, Maria Magliulo1,2, Antonia Mallardi3,

Gianluca Lattanzi1,2, Krishna Persaud4, Luisa Torsi1,2,

1University of Bari, Italy, 2CSGI, Italy,

3CNR-IPCF, Italy, 4University of Manchester, UK.

1

Colloidal, Macromolecular & Biological Gels: Formulation, Properties & Applications

July 10 - 14 2016 Hernstein, Austria

point-of-care (POC) testing: clinical tests to be performed at the site of patient care

Sensors: Portable, cheap (disposable) and easy to operate

2

OFET = Organic Field Effect Transistor

3

Why organic electronics ?

Wereable sensors

Flex plastic substrate

Low cost

Large area

Organic electronics @UNIBA

Organic field-effect transistor OFET

Gate (G)

dielectric

Vgs

Dielectric layer

drain S

source

D

20 0 -20 -40 -60 -80 -100

0

-10

-20

-30

-40

-50

-60

I ds(

A)

Vg(V)

4

Organic semiconductor

drain

S D Bio receptor layer D

analyte

Vds

OFET biosensor

Response = I/I0

5

Bao’s group @Stanford

Thrombin sensor LOD 100 pM Hammock et al. ACS NANO 2013, 7, 3970

glial fibrillary acidic protein (GFAP) sensor LOD 1 ng/mL = 20 pM Huang et al. Chem. Sci. 2014, 5, 416

Katz group @Johns Hopkins University

Top-contacts bottom-gate

6

J. Mater. Chem. C, 2015,3, 6445

Angew. Chem. Int. Ed. 2015, 54, 12562

How does it work?

7

2)(2

TGFETDS VVCL

WI VT=voltage threshold

Depends on chem. Pot charge carriers

It is affected by electrically charged analytes

Dielectric layer capacitance ???

OFET detections are possible only for: 1) charged analytes 2) at salt concentration low enough so

that the Debye’s length is larger than the analyte size.

good performance requires high capacitances, i.e. high-k dielectrics

in form of very thin films

How does it work?

OSC source drain VDS

EGOFET

electrolyte-gated field-effect transistor: An alternative approach to high-capacitance gate dielectric

+ + + +

electrolyte

⊖ ⊖ ⊖ ⊖

gate

VG

Heeger, Phys. Rev. Lett. 2006, 96, 246403. Panzer & Frisbie, Appl. Phys. Lett 2006, 88, 203504

8

Helmholtz double layer (HDL)

- - - -

Porcine Odorant Binding Protein (pOBP)

Y. Mulla

Porcine Odorant Binding Protein (pOBP)

Krishna Persaud e Elena Tucconi

The University of Manchester,

9

Spearmint Smell Caraway smell

S(+)-

Carvone R(-)-

Carvone

• Shuttle odorant molecules

• Soluble proteins, can be expressed in

bacterial systems at low-cost

• Highly stable

19 kDa

100101102103104105106

- 0.0

- 0.2

- 0.4

- 0.6 (S)-(+)-carvone

(R)-(-)-carvon

I/

I 0

[ligand] (pM)

10

Sensitive biosensing (LOD 100 pM) of electrically neutral analytes

What is going on? Carvone 150 Da; pOBP 19 KDa

10010

110

210

310

410

510

6

-0.0

-0.1

-0.2

-0.3

-0.4

-0.5 (S)-(+)carvone

(R)-(-)carvone

C

/C

[ligand] (pM)

The response is dominated by capacitance

11

MD simulations of pigOBP F88W

PDB code: 1E00 System size: ~ 46278 atoms. pH: ~ 5.5 Force field: CHARMM27 + TIP3P water. Cutoff van der Waals: 12 Å. Electrostatic interactions: PME with direct sum cutoff at 12 Å. Constraints: SHAKE for all R-H bonds Time step: 2 fs NAMD 2.9 on FERMI supercomputer @CINECA

NPT ensemble (298 K, 1 atm) with Nosè-Hoover Langevin barostat (oscillation period 200 fs, decay coefficient 100 fs) and Langevin thermostat (damping coefficient 1 ps-1). Total simulation time: 25 ns

G. Lattanzi

• Only a single state can be defined for S (+) carvone:

Interaction Planarity of carvone

• Two different states can be defined for R (-) carvone:

Interaction Planarity Interaction

Planarity

R* R*

chiral atom

chiral atom

reorientation

The complex pOBP-carvone is different for S(+) and R(-) carvone

high dielectric percolative path, “water channel”

R(-)-Carvone 𝐶𝑂𝐵𝑃 ≃ 𝐶𝑤

S(+)-Carvone 𝐶𝑂𝐵𝑃 = 𝐶𝑝

A CHANGE 2.4 % of the total surface of the protein ACCOUNTS FOR THE

OBSERVED RESPONE

13

R S

The response is dominated by capacitance

14

a minute change in protein layer capacitance modulate a water-gated OFET, allowing for chiral differential detection with large

enantiomeric discrimination factor

neutral ligand detection in the picomolar concentration range.

For details

NATURE COMMUNICATIONS |2015, 6:6010 |

SUMMARIZING

Insight on the energy of ligand binding to immobilized proteins

OSC source drain VDS

EGOFET

electrolyte-gated field-effect transistor: An alternative approach to high-capacitance gate dielectric

+ + + +

electrolyte

⊖ ⊖ ⊖ ⊖

gate

VG

Heeger, Phys. Rev. Lett. 2006, 96, 246403. Panzer & Frisbie, Appl. Phys. Lett 2006, 88, 203504

HDL

HDL

GCDL

GCDL

Good EGOFET performances require short Debye’s length

15

Helmholtz double layer (HDL)

- - - -

𝐶𝐺𝐶𝐷𝐿 =𝜀𝜀0

𝜆∝ 𝑖𝑠

10F/cm2

This is an issue in biosensing

the Debye’s screening length is the length-scale at which a charged

analyte can be electrically probed at the detector interface.

Hammock et al. 2013, ACSnano, 5, 3970

16

No detection when

< the distance at which the

recognition event takes place

OFET detections should be possible only at salt concentration low enough so that is larger than the analyte size

Large means small gate capacitance = unperforming OFET and this should be prejudicial for the use of EGOFETs as biosensors.

BUT

2013-2014: workable sensing at a distance larger than are reported Magliulo et al. Adv. Mater. 2013, 25, 2090 [ionic strength=0.16 M =0.7 nm] Huang et al. Chem. Sci. 2014, 5, 416 [ionic strength=0.08 M =3 nm] Knopfmacher et al. Nature Comm., 2014, 5 art. 2954 [sea water]

Need for a systematic study of a sensor response as a function of the Debye’s length and the distance at which the binding event takes place.

17

scheme of phospholipid BIOEGOFET fabrication

PE-CVD Acrylic acid + ethylene +argon

PL-OSC conjugation 1) EDC-NHS

2)Phosphatidylethanolamine

BIOEGOFET

OSC

COOH COOH COOH COOH

substrate Gold contact

Spin coating

OSC

OSC

⃝ −

+ + + +

⃝ − ⃝ − ⃝ −

gate

Source Drain

- - - -

0.0 -0.1 -0.2 -0.3 -0.4 -0.50.0

-0.2

-0.4

-0.6

-0.8

I DS (

A)

VDS

(V)

18

30 nm

5 nm

20 nm

Streptavidin (SA) binds to biotin

Biotinylated Antibody (aB) against CRP

aB is bound by the SA

C-reactive protein (CRP) is the antigene of the aB

Tuning the distance at which the binding event takes place

19 Tuning : dilution

Response = I/I0 = (IDS-I0)/I0 In PBS !!

20

IDS

I0

PBS Ionic strength = 0.160 M = 0.7 nm To tune : dilution

0,0 -0,2 -0,40,00

-0,05

-0,10

-0,15

I DS /A

VG /V

Serum+CRP 10 g/ml

Serum+CRP 1 g/ml

Serum

serum

CRP sensing in human serum

21

Debye’s length

The sequential binding of the three proteins is reproducibly probed at salt concentration typical for human blood

???

20 30 40 50 60 70 809010 100

-0.3

-0.2

-0.1

0.0

I/I0fractional change

antibody concentration /g mL

-1

Antibody binding to PL/SA

2)(2

TGFETDS VVCL

WI

∆𝑰

𝑰𝟎=

∆𝐂

𝑪𝟎+

𝟐∆𝑽𝑻

𝑽𝑮 − 𝑽𝑻,𝟎

the response to the analyte is mainly capacitive

2VT/|V

G-V

T,0|

C/C0

22

1 2 3 4 5 6 7 8 910 20 30 40 501 10-0.2

-0.1

0.0

0.1

0.2

0.3

0.4

0.5

CRP concentration /g mL

-1

fra

ctio

na

l re

sp

on

se

I/I0

CRP binding to PL/SA/Ab

2VT

/|VG

-VT,0

|

C/C0

22

CRP binding to PL/SA(AV)/Ab

The charges on the protein backbone are fixed . the free counterions cannot leave the region of the fixed charges for distances > (electroneutrality ): Donnan’s equilibrium.

23

an electrical double layer is formed at the boundary of the fixed ions region

H. Ohshima Sci. Technol. Adv. Mater. 2009, 10, art. 063001 Ohshima H Theory of Colloid and Interfacial Electric Phenomena, Elsevier/Academic Press, New York, USA 2006

The capacitance of the Donnan’s double layer is proportional to the ionic strength (CDONis)

M. Borkovec, B. Jönsson, G.J.M. Koper in Surface and Colloid Science, Vol. 16 (Ed. E. Matijevic) p.99 Kluwer, New York, USA 2001, Ch.2

Why the capacitance changes??

Overall the gating capacitance C can be described as:

𝐂 =𝟏

𝑪𝒇𝒊𝒙+

𝟏

𝑪𝑮𝑪𝑫𝑳+

𝟏

𝑪𝑫𝑶𝑵

−𝟏

+ 𝑪𝒑𝒂𝒓

The binding adds a new layer that changes the capacitance impacting on the 1/CDON

24

the bio-EGOFET response is governed by a capacitive effect that is independent from the position at which the Donnan’s equilibrium is set and therefore does not depend on the Debye’s length.

To test this hypothesis the dependence from the ionic strength of the capacitance was studied

0.01 0.1 1 10 100

-0.8

-0.6

-0.4

-0.2

0.0

PL

PL-SA-aB

PL-SA-aB

C

/C0

I (mM)

PL

PL-SA-aB

PL-SA-aB-CRP

15 nm

25 nm

∆𝑪

𝑪𝟎=

𝑪𝟎

𝑪𝒇𝒊𝒙+

𝑪𝟎𝑲𝑻

𝒆𝟐𝜺𝜺°

𝒊𝒔

+𝑪𝟎𝒈−𝟏

𝒊𝒔

−𝟏

+𝑪𝒑𝒂𝒓

𝑪𝟎− 𝟏

25

capacitive tuning of the EGOFET response on gate

CRP in PBS @ fM

10-16

10-14

10-12

10-10

10-8

10-6

-0.2

-0.4

-0.6

-0.8

-1.0Streptavidin-AntiCRP: CRP sensing

I/

I 0

[CRP] (M)

4 fM

not-published data 26

summarizing, • EGOFET sensors, can probe a protein binding taking place at

more than 30 far from the transistor channel.

• The mechanism of sensing is mainly capacitive and is due to the formation of Donnan’s equilibria within the protein layer.

• This capacitive tuning of the EGOFET response is virtually insensible to the Debye’s length value.

27

For details

M. Y. Mulla

A. Mallardi

28

Message to take –home

The mechanism of transduction of the molecular recognition in EG-OFET relies on the electrostatic properties of soft matter

Financial support

29