Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration...

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Electronique Electronique mol mol é é culaire culaire : : é é tat tat de de l'art l'art & perspectives & perspectives D. Vuillaume Institute for Electronics, Microelectronics & Nanotechnology – CNRS, Lille “Molecular Nanostructures & Devices” group SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped Al SiO 2 1nm Si highly doped hydrogen carbon oxygen sulfur silicon Au Au -(CH 2 ) 3 -SH or C3-SH -(CH 2 ) 3 -CH 3 or C3 -(CH 2 ) 6 -CH=CH 2 or C8 1.0μm

Transcript of Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration...

Page 1: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

Electronique Electronique molmol ééculaireculaire ::éétattat de de l'artl'art & perspectives& perspectives

D. VuillaumeInstitute for Electronics, Microelectronics

& Nanotechnology – CNRS, Lille“Molecular Nanostructures & Devices” group

SiO2 1nm Si highly doped

SiO2 1nm Si highly doped

Al

SiO2 1nm Si highly doped

hydrogen carbon oxygen

sulfur

silicon

Au Au

-(CH2)3-SH or C3-SH -(CH2)3-CH3 or C3 -(CH2)6-CH=CH2 or C8 1.0µm

Page 2: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

PlanPlan

• Définition, quelques repères historiques

• Principes de base, structure et transport électroniquedans une jonction moléculaire

• Exemples de composants à l'échelle moléculaire

Page 3: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

Definition, introduction, Definition, introduction, foundations of the fieldfoundations of the field

Page 4: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

• “Information processing using photo-, electro-, iono-, magneto-, thermo-, mechanico or chemio-active effects at the scale of structurally and functionally organized molecular architectures”

(Adapted from: J.M. Lehn, Angew. Chem. Int. Ed., 1988, Noble Lecture)

Molecular Electronics - manipulate and control the position of one or few molecules- tailor their electronic properties to obtain useful devices

1 molécule - 1 monocouche

Page 5: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

Pioneer resultsPioneer results

M1 A D M2

Fermienergy

LUMO

HOMO

LUMO

HOMO

Aviram-Ratner proposal

Aviram & Ratner, Chem Phys Lett (1974)IBM, New York U.

Theoretical suggestion of amolecular analog of the p-n junction:the donor-bridge-acceptor molecularjunction.

A - σ - D

Page 6: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

1rst evidence of tunnelingthrough a fatty acid LBmonolayer sandwichedbetween metal electrodes

Mann & Kuhn, JAP (1971)MPI

Page 7: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

Dimension

Courtesy of J.P. Bourgoin (LEM-CEA)

Page 8: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

Basic problems : electronic structure, Basic problems : electronic structure, basic devices and electronic transportbasic devices and electronic transport

Page 9: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

Molecule vs.Molecule vs.MetalMetal --MoleculeMolecule --Metal junctionMetal junction

« L'électronique moléculaire », J.P. Bourgoin, D. Vuillaume, M. Goffman & A. Filoramo.In "Les nanosciences, nanotechnologies et nanophysique", eds. M. Lahmani, C. Dupas P. Houdy (Belin, Paris, 2004), pp.400-449

•hybridation•charge transfer

0

E

V

Page 10: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

Vondrak et al., J. Phys. Chem B (1999)

Page 11: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

single molecule single molecule →→→→→→→→ ensemble of moleculesensemble of molecules

Page 12: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

Charge transport, currentCharge transport, current --voltagevoltage

1µ2µ

Low bias:tunnel effect

1µ2µ

Higher bias:resonancethrough MO

gVe=− 21 µµ

low coupling

Page 13: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

V

I

V

I

C. Joachim et al. Phys. Rev. Lett. 74, 2102 (1995)Europhys. Lett. 30, 409 (1995)

D. Porath et al.J. Appl. Phys. 81, 2241 (1997)Phys. Rev. B 56, 9829 (1997)

Page 14: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

control of the electrodecontrol of the electrode --molecule interface is molecule interface is crucialcrucial

Li et al., JACS (2006)Arizona U.

2.5x10-4G0

0.5x10-4G0

Patrone et al., Chem Phys (2002) LEM-CEA

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What can we do with molecules ? What can we do with molecules ? Which types of electronic devices?Which types of electronic devices?

Page 16: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

electronic function in moleculeselectronic function in molecules

S

SS

S

SS

CN

CNNC

NC16H33

semiconductor/metal

rectifyier

insulator

bistable, memory

switch

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tunnel barriertunnel barrier

3.0 3.5 4.0 4.5 5.0 5.5 6.0 6.5 7.0

-1.0x10-14

0.0

1.0x10-14

2.0x10-14

3.0x10-14

4.0x10-14

5.0x10-14

6.0x10-14

7.0x10-14

Flux signal (V

)

Pho

tocu

rren

t (A

)

Photon energy (eV)

HTS DTS OTS

3.0 3.5 4.0 4.5 5.0 5.5 6.0 6.5 7.0

10-3

10-2

10-1

100

flux

D. Vuillaume et al., Phys. Rev. B (1998), Phys Rev. Lett. (1996)

A. Salomon et al., PRL (2005); Adv Mater (2007)

1.5 2.0 2.5 3.0

1x10-8

1x10-7

1x10-6

1x10-5

1x10-4

1x10-3

Monolayer thickness (nm)

Cur

rent

den

sity

(A

/cm

2 )

•E.E. Polymeropoulos et J. Sagiv, J. Chem. Phys. (1978)•C. Boulas et al., Phys. Rev. Lett. (1996)•J. Holmlin et al., J. Am. Chem. Soc. (2001)•D.J. Wold et al., J. Am. Chem. Soc. (2000,2001)•X.D. Cui et al., J. Phys. Chem. B (2002)

∆∆?

Au-S- : ~ 1.5 - 2.5 eVSi-C- : ~ 1.5 eV

Si-O- : ~ 4 - 4.5 eV

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S. Lenfant et al. Phys. Stat. Sol. a (2006), IEMN-CNRSKushmerick et al. Nano Lett. (2004), NISTWang et al. Nano Lett? (2004), Yale

Couplage electron-vibration moléculaireIETS

fluctuations, bruit

SiO2 1nm Si highly doped

SiO2 1nm Si highly doped

Al

SiO2 1nm Si highly doped

hydrogen carbon oxygen

sulfur

silicon

Au Au

-(CH2)3-SH or C3-SH -(CH2)3-CH3 or C3 -(CH2)6-CH=CH2 or C8

localized (E,z) defects

N. Clement et al., PRL (soumis)IEMN-CNRS & Weizmann

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molecular rectifying diodemolecular rectifying diode

D A

-2 -1 0 1 2

0

2x10-3

4x10-3

6x10-3

8x10-3

1x10-2

(a)LB3/5,chena/bo429d

Cur

rent

den

sity

(m

A/c

m2 )

Voltage (V)

CN

CNNC

NC16H33

Aviram & Ratner concept (1974)

A.S. Martin et al., Phys. Rev. Lett. (1993), Cranfield U.

R.M. Metzger et al., J. Am. Chem. Soc. (1997), Alabama U.

D. Vuillaume et al., Langmuir (1999), IEMN-CNRS

RR~30V>0

DA

Page 20: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

simplified concept

-1.0 -0.5 0.0 0.5 1.0-2.5x10-5

-2.0x10-5

-1.5x10-5

-1.0x10-5

-5.0x10-6

0.0

5.0x10-6

1.0x10-5

OETS-thiophene HETS-phenyl HETS-thiophene

VT

Cur

rent

den

sity

(A

.cm

-2)

Voltage (V)S. Lenfant et al., Nano Letters (2003)D. Vuillaume, J. Nanosci. Nanotechnol. (2002)S. Lenfant et al., J. Phys. Chem. B (2006)IEMN-CNRS

Π

RR~37

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capacitive molecular memorycapacitive molecular memory

+∆Q

∆I∆V∆…

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U. California Riverside, North Carolina & ZettaCore Inc (2002) Liu et al., science (2003)

PorphyrinPorphyrin --based SAM on Sibased SAM on Si --H surfacesH surfaces

multi-redox = multi-valuedwrite ~ 10-3 - 10-5 srentention ~ 100-200 sr/w cycle : 1012

stable : 400°C (30min, inert atm)charge density ~16 µC/cm2

Kuhr et al., MRS Bul (2004)

Page 23: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

MMéémoiremoire molmol ééculaireculaire capacitivecapacitive

SiSiO2, 2 nm

C60, 1ML

Al2O3 (ALD), 30 nmSiO2 (PECVD), 26 nm

Hou et al., APL (2006)Cornell

Page 24: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

functionalized NW memoryfunctionalized NW memory

Duan et al., Nano Letters (2002) Harvard Univ

InP (10-30 nm) + Co phthalocyanine

on/off ~104

write ~ ?? srentention ~ 20min -600hr/w cycle : ??stable : ??

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resistive molecular memoryresistive molecular memory

Ron Roff

command

Page 26: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

S

S

SSHSH

Gplane > Gtwisté

G ~ G0 cos2θ

SSSHSH

S

Page 27: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

Vankataraman et al., Nature (2006)Columbia

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several attemptsseveral attempts ……

A. Szuchmacher Blum et al.,Nature Mater. (2005)NRL, Rice, Geo-Centers

Moore et al.JACS (2006)Penn State & Rice U.

Donhauser et al., Science (2001)Penn State & Rice U.

Au(111)/mica

Page 29: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

avoid thiol on gold !avoid thiol on gold !

~8.3eV~800kJ/molSi-O

less sensitive to local structurecoupling through N lone pair

NH2/Au

~4.7eV~451kJ/molSi-C

~3.3eV~326kJ/molSi-Si

~1.8eV~180kJ/molAu-S

Page 30: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

Very low energy

Loppacher et al., PRL (2003)U. Basel, IBM & CEMES-CNRS

~50zJ

θ=10°"OFF"

θ=55°"ON"

F. Moresco et al., Phys. Rev. Lett. (2001)U. Berlin & CEMES-CNRS

- CMOS FET : 0.1-1 fJ

- mol switch : 50 zJ

- kTLn2=2.8 zJ (@300K)

1012 "devices" at 1 GHz = 47 W

~ x104

~ x20

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molecular transistormolecular transistor

McEuen & Ralph et al. Nature 2002Cornell

20-60 nm

Mottaghi et al. Adv Func Mater. (2007)ITODYS, IEMN-CNRS

Park et al, Nature 2002Harvard

Coulomb blokadeKondo effect

field effect

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other molecular devicesother molecular devices

McEuen & Ralph et al. Nature 2002Park et al, Nature 2002

N. P. Guisinger et al, Nanoletters 4, 55 (2004)

Feringa et al., Adv. Mater. (2006)Univ. Groningen

NDR diodeMolecular transistor

Optical switch

Molecular spin-valve

Ralph et al., Phys Rev Lett (2004)

Page 33: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

molecularmolecular --based circuitsbased circuits

J.M. Tour et al., IEEE Trans Nanotechnol. (2002)J.M. Tour et al., J. Am. Chem. Soc. (2003)

"NANOCELL"

A. Dehon et al., IEEE Trans Nanotechnol. (2003)

"Connecting nano to micro"

Crossnets Synaptic plaquette

Lykharev (2004)

NanoBlocks and NanoFabrics

Goldstein (2001)

Page 34: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

Conclusions and perspectivesConclusions and perspectives

• Several functions and devices have been studied at the molecular scale : tunnel barrier, molecular wire, rectifying and NDR diodes, bistable devices and memories.– A better understanding and further improvements are

mandatory.– Need to be confirmed– What's about a true molecular 3-terminals device?

• Molecule-electrode coupling and conformation strongly modifies the molecular-scale device properties. Molecular engineering (changing ligand atoms for example) may be used to improve or adjust the electrode-molecule coupling.– A better control of the interface (energetics and atomic

conformation) is still compulsory.

Page 35: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

• Towards molecular architecture and circuits: mainly the « cross-bar » architecture has been studied. Is it sufficient?– More new architectures must be explored (e.g. non Von

Neuman, neuronal…).– Molecular device interconnection?– 3D

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Page 37: Electronique mol éculaire : état de l'art & perspectives · Couplage electron-vibration moléculaire IETS fluctuations, bruit SiO 2 1nm Si highly doped SiO 2 1nm Si highly doped

Thank you!Thank you!