superconductivity in moth balls: surprises in organic transistors april 10, 2002 jairo sinova ref:...
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Superconductivity in moth balls:
surprises in organic transistors
April 10, 2002Jairo Sinova
Ref: J. Sinova et al, Phys. Rev. Lett. 87, 226802 (2001)
Financial support by
OUTLINE
• Introduction to organic thin film transistors
• Experimental surprises
• Quantum confinement in organic thin films
• Superconductivity in organic materials: electron-phonon coupling
• Comparison to experiments
• Conclusion
OUTLINE
• Introduction to organic thin film transistors– Organic field effect transistors (FETs)– Future and present applications of plastic electronics– Materials used in organic field effect transistors and their
properties
• Experimental Surprises in the past year• 2-D electron transport in organic thin films• Superconductivity in organic materials: electron-
phonon coupling• Comparison to experiments• Conclusion
Organic Field Effect Transistors
J. H. Schön, S. Berg, Ch. Kloc, and B. BatloggScience 2000 February 11; 287: 1022-1023
substrate
semiconductor
insulatorS Dgate
Vg
thin free charge carrierchannel induced by
electric field from gate
- - - - - -
>0
• Density of carriers proportional to gate voltage: changes in VG have a dramatic change in channel conductance (important technologically)
High mobility 2DEG: IQHE, FQHE, MIT, etc.
Applications of plastic transistors: future and present
LEDs plastic display
Cheaper solar cells
All plastic RAMS?
Printing plastic transistors and organic LEDs
C60
MATERIALS USED IN ORGANIC FETs
PentaceneTetracene
AnthracenceNaphthalene: moth balls
The aromatic molecules: polyacenes
ALSO:
SSS
SS
S
-6T
SS
SS
-4T
Tc=117 K!!
Material Properties of the Polyacenes and organic semiconductors
Energy levels of individual molecules
LUMO
HOMOE
Narrow bands in molecular crystal
(extended (delocalized) -electrons)
~ 1.5 -3 eV
•Lower mobility than silicon•Soft and flexible (Van-der-Waals bonding)•Larger size molecules: richer vibration spectrum (polaron rich)•Narrow bands: low overlap of conducting orbitals (contrast with metals and silicon); low T•Heavier carrier masses•Polaron physics at higher T
OUTLINE
• Introduction to organic thin film transistors• Experimental Surprises in the past year
– 2-D transport experiments in polyacene FETs– What are the key surprises?– Superconductivity: experimental finding
• 2-D electron transport in organic thin films• Superconductivity in organic materials: electron-
phonon coupling• Comparison to experiments• Conclusion
experiments by Batlogg, et al; courtesy of Dr. A. Dodabalapour
0.45 0.50 0.55 0.60 0.65 0.70 0.7510
-2
10-1
100
101
102
c
Insulator : =cexp((To/T)1/2
)
Metal : =cexp(-(To/T)1/2
)
holes / Pentacene MOSFET
T-0.5 (K-0.5)
(h/
e2 )
MIT
109
1010
1011
1012
1013
1014
p / cm-2
2DEG in Organic FETs: physical effects galore
2D Electron/Hole Gas
Gate
source and drain
gate insulator (Al2O3)
increasing voltage
0 2 4 6 80
20
40
60
80
100
Tetracene(Holes / 1.7 K)
5x1010
cm-2
6x1010
cm-2
7x1010
cm-2
8x1010
cm-2h/3e2
h/2e2
3h/e2
5h/2e2
3h/2e2
h/e2
Magnetic Field (T)
Rxy (k)
FQHE
0 2 4 6 80
20
40
60
80
100
Tetracene(Holes / 1.7 K)
5x1010
cm-2
6x1010
cm-2
7x1010
cm-2
8x1010
cm-2h/3e2
h/2e2
3h/e2
5h/2e2
3h/2e2
h/e2
Magnetic Field (T)
Rxy (k)
FQHE
0 2 4 6 80
5
10
15
20
25
30 Pentacene
1.7 K
Magnetic Field (T)
Resi
stance
R xx,
Rxy (
k)
IQHE
IQHE
0 2 4 6 80
5
10
15
20
25
30 Pentacene
1.7 K
Magnetic Field (T)
Res
ista
nce
Rxx
, Rxy
(k
)
0 5 10 15 20 25
1.8
2.0
2.2
2.4
2.6
2.8
3.0
3.2
Resistance
Ballistic Holes in Pentacene
Magnetic Field (mT)
Te
mp
era
ture
(K
)
MF
0 5 10 15 20 25
1.8
2.0
2.2
2.4
2.6
2.8
3.0
3.2
Resistance
Ballistic Holes in Pentacene
Magnetic Field (mT)
Tem
pera
ture
(K
)
MF
0.45 0.50 0.55 0.60 0.65 0.70 0.7510
-2
10-1
100
101
102
c
Insulator : =cexp((T
o/T)
1/2)
Metal : =cexp(-(T
o/T)
1/2)
holes / Pentacene MOSFET
T-0.5
(K-0.5
)
(h
/e2 )
MIT
100 110 120 1301.7
1.8
1.9
2.0
2.1
2.2
2.3
2.4
2.5
Resistance
Superconducting State
Normal State
Gate Voltage (V)
Tem
pera
ture
(K
)
0.85 0.90 0.95 1.00 1.05
Electrons per Molecule
100 110 120 1301.7
1.8
1.9
2.0
2.1
2.2
2.3
2.4
2.5
Resista
nce
Superconducting State
Normal State
Gate Voltage (V)
Tem
pera
ture
(K
)
0.85 0.90 0.95 1.00 1.05
Electrons per Molecule
SC
2.0 2.5 3.0 3.5 4.0 4.50.0
0.2
0.4
0.6
0.8
1.0
Anthracene
Pentacene
Tetracene
Temperature (K)
Res
ista
nce
(a.u
.)
J. H. Schön et al. Nature 406, 702 (2000)
Increase of Tc
with decreasingmolecular size
Similar behaviorfor oligothiophenes
(-4T, -6T, and -8T)
J. H. Schön et al. Phys Rev. B 64, 035209 (2001).
Gate-Induced Superconductivity in Polyacenes
courtesy of Dr. A. Dodabalapour
100 110 120 1301.7
1.8
1.9
2.0
2.1
2.2
2.3
2.4
2.5
Resistance
Superconducting State
Normal State
Gate Voltage (V)
Tem
pera
ture
(K
)
0.85 0.90 0.95 1.00 1.05
Electrons per Molecule
J. H. Schön et al. Nature 406, 702 (2000)
Electron-doping(~ 1014 cm-2)
80 - 100 Å
no bulksuperconductivity
Gate-Induced Superconductivity in Pentacene
courtesy of Dr. A. Dodabalapour
Electron-Phonon coupling strength spectrum experiments
M. Lee, et al, PRL 86, 862 (2001)
Infrared absorption
Conductance derivative spectrum of a
pentacene-Pb tunnel junction
Questions and Puzzles
• How can so many effects occur in one single sample?
• How 2-d is the quantum confinement?• What electron-phonon coupling drives the
superconductivity?• Is the FQHE regime highly interacting?• Is the vibrational spectrum affected by the
injected electrons?• Is this behavior generic to all organic materials?
...
OUTLINE
• Introduction to organic thin film transistors• Experimental Surprises in the past year • 2-D electron transport in organic thin films
– Self-consistent calculation of the electronic structure– How two dimensional is the system? How many sub-
bands are occupied?
• Superconductivity in organic materials: electron-phonon coupling
• Comparison to experiments• Conclusion
1.3 eV
valence band
conduction band
VG=0
How confined are the carriers at the interface?:2D or not 2D
Model calculation:
local density self consistent mean field calculation of the bands (continuous)
Important parameters:dielectric constants, density of carriers, lattice constant,insulator-semiconductorgap difference.
VG
organic semiconductor(anthracene)
Al2O3Au
1.3 eV
valence band
conduction band
VG>0
0 1 2
nm
0 1 2
nm
OUTLINE
• Introduction to organic thin film transistors• Experimental Surprises in the past year • 2-D electron transport in organic thin films• Superconductivity in organic materials: electron-
phonon coupling– General BCS superconductivity– Model: what type of electron-phonon to consider?– Vibrational spectrum calculation
• Comparison to experiments• Conclusion
Superconductivity: B-C-S• In normal superconductors electrons form pairs (Cooper
pairs)– Phonon assisted, carriers have opposite spins – Cooper pairs follow B-E statistics and a ‘condensation’ leads to SC
SC in organic (polyacenes) materials
•2D electrons-3D phonons•non-standard e-ph coupling•Rich vibrational spectra
2D Electron/Hole Gas
Gate
source and drain
gate insulator (Al2O3)
AB
Modeling electron-phonon coupling in anthracene
extvibreeKEtotal HHHHH
vibrDKEsiteontotal HHHH 2
after the LDA/Hartree calculation this reduces to
Su-Schrieffer-Heeger coupling
0KE
H phonelecH
Ruu
ttrt m
mm
~~,
6
1 2,10
ii
eei
HOMOi n)(
On the omission of the Holstein term
A. Devos and M. Lannoo, PRB 58, 8236 (1998)
non-degenerate LUMO/HOMO level
no elec-phon couplingwhen screening is present
This is NOT the case in fullerenes where the Holstein term is dominant and the SSH term is much smaller
Molecule DegenUnscreened
Holstein Coupling (meV)
Screened Holstein
Coupling (meV)
Anthracene L(1) 166 0
Tetracene L(1) 130 0
Pyrene L(1) 197 0
C60 L(3) 52 47
C28 H(3) 80 80
C20 H(4) 183 183
uu
eeiii
)(
A8A4 FTF l
3D Phonon Spectrum
phonon spectrumdispersion calculation
J. Sinova et al, PRL 87, 226802 (01)
Atom-Atom potential modelusing the Williams’ parametersto obtain the secular equation
)q,q)D)q,q,
((,()(2 inn
n
imi
Taddei, et al., J. Chem. Phys. 58, 966 (73)Dorner et al., J. Phys. C 15, 2353 (82)
2D electron-3D phonon term
kq]kQ,Q,
-Qk
Qk
,[,
BZ3D
,
,BZ-2D
ˆˆ]ˆˆ[,,(1
iiji
ji
vibe ccaaN
H
††g
))1((,()'(
(~
22
~)1(,q,(
')('[
,,' ,
,z,
kk]qqQ
Q)q,k
ijiiim
m
m m
iji
eeeu
t
M
fg
Calculation of mu
t
)(
•assume t is proportional to orbital overlap•
•obtain orbitals using the Hückel approximation
0)( tu
tm
0.4
0.6
0.8
1
1.2
-1.2 -0.8 -0.4 0 0.4 0.8 1.2
orbi
tal o
verla
p
n.n. distance
OUTLINE
• Introduction to organic thin film transistors
• Experimental Surprises in the past year
• 2-D electron transport in organic thin films
• Superconductivity in organic materials: electron-phonon coupling
• Comparison to experiments– Electron-phonon coupling calculation, Tc calculation
– Agreement and predictions
• Conclusion/Final message
n2d~0.2-0.7/mol
Calculation and experiment comparison
M. Lee, et al, PRL 86, 862 (2001)
calculation
experiments
100 110 120 1301.7
1.8
1.9
2.0
2.1
2.2
2.3
2.4
2.5
Re
sis
tan
ce
Superconducting State
Normal State
Gate Voltage (V)
Te
mp
era
ture
(K
)
0.85 0.90 0.95 1.00 1.05
Electrons per Molecule
J. H. Schön et al. Nature 406, 702 (2000)
J. Sinova et al, PRL 87, 226802 (01)
n2d~1/mo
A
A
B
B
C
C
Tc~2 K
/1 eT Dc
DOS and SC relations: injected carrier density trends
•Rounded by disorder•SC will go away if p increases beyond half filling
100 110 120 1301.7
1.8
1.9
2.0
2.1
2.2
2.3
2.4
2.5
Resistance
Superconducting State
Normal State
Gate Voltage (V)T
empe
ratu
re (
K)
0.85 0.90 0.95 1.00 1.05
Electrons per Molecule
Model Calculation Results and Predictions
•Shows the sharp onset of SC with gate voltage•Agreement with peaks observed in absorption/tunneling experiments•Correct order of Tc (~2K compared with ~3K in experiments)•Tc should increase with pressure (with t0) in contrast with the fullerenes• SC will disappear as p goes beyond half filling in single band FET organic semiconductors
UPDATE FROM MM 02: C. Kloc
Not same material but similar SC physics
A Final Message From The Prophetic Mr.McGuire
Alvaro S. NuñezJohn Schliemann
Allan H. MacDonaldTomas Jungwirth
work done in collaboration with
100 110 120 1301.7
1.8
1.9
2.0
2.1
2.2
2.3
2.4
2.5
Resistance
Superconducting State
Normal State
Gate Voltage (V)
Tem
pera
ture
(K
)
0.85 0.90 0.95 1.00 1.05
Electrons per Molecule
0 5 10 15 20 25
1.8
2.0
2.2
2.4
2.6
2.8
3.0
3.2
Resistance
Ballistic Holes in Pentacene
Magnetic Field (mT)
Tem
pera
ture
(K
)
Mr. McGuire was right:there is a future in plastics
109
1010
1011
1012
1013
1014
0 2 4 6 80
20
40
60
80
100
Tetracene(Holes / 1.7 K)
5x1010
cm-2
6x1010
cm-2
7x1010
cm-2
8x1010
cm-2h/3e2
h/2e2
3h/e2
5h/2e2
3h/2e2
h/e2
Magnetic Field (T)
Rxy (k)
0.45 0.50 0.55 0.60 0.65 0.70 0.7510
-2
10-1
100
101
102
c
Insulator : =cexp((To/T)1/2
)
Metal : =cexp(-(To/T)1/2
)
holes / Pentacene MOSFET
T-0.5 (K-0.5)
(h/
e2 )
100 110 120 1301.7
1.8
1.9
2.0
2.1
2.2
2.3
2.4
2.5
Resistance
Superconducting State
Normal State
Gate Voltage (V)
Tem
pera
ture
(K
)
0.85 0.90 0.95 1.00 1.05
Electrons per Molecule
FQHE
IQHE
MIT
SC0 5 10 15 20 25
1.8
2.0
2.2
2.4
2.6
2.8
3.0
3.2
Resistance
Ballistic Holes in Pentacene
Magnetic Field (mT)
Tem
pera
ture
(K
)
0 2 4 6 80
5
10
15
20
25
30 Pentacene
1.7 K
Magnetic Field (T)
Res
ista
nce
Rxx
, Rxy
(k
)
MFp / cm-3
2DEG in Organic FETs: physical effects galore
2D Electron/Hole Gas
Gate
source and drain
gate insulator (Al2O3)
increasing voltage
experiments by Batlogg, et al
Mermin-Wagner Theorem: an academic exercise in a MF regime
KTT
No true long range order in 2-DThermal and quantum fluctuations destroy it
In a mean field regime these fluctuations are very smalland superfluid-stiffness very large
10 100 50010-1
100
101
102
103
T-2.8
T-2.3
T-1.8
Pentacene
Temperature (K)
Mob
ility
(cm
2 /Vs)
3D Band Transport
High T (~ 400 K) :Crossover to
Hopping
Anisotropy (Pentacene)
2.0 2.5 3.0 3.5 4.010
-2
10-1
100
101
102
increasing n
Pentacene / MOSFET electrons
Temperature (K)
(h/
e2 )
Metal-Insulator-Transition in 2DElectron Density :61010 - 51011 cm-2
Peak mobility :2104 cm2/Vs
Critical Concentration :pc 3.21011 cm-2
Strong El.-El. Interact.m* ~ 1.5 me
eff ~ 6
Magneto-Phonon Effect m*(T)
0 2 4 6 8 10 12 14 160.0
0.1
0.2
0.3
40 K 60 K 80 K
2me
1.7me
1.5me
Tetracene (Holes : 2x1011 cm-2)
N
1/B
(1/
T)
4 6 8
60 K
40 K
B (T)
-d2 R
/dB
2 (ar
b. u
nits
) Resonant Scattering of Charge Carriersbetween Landau-Levels
by LO-Phonons
V. L. Gurevich and Y. A. Firsov, Zh. Eksp. Teor. Fiz. 40, 198 (1961)
(Sov. Phys.JETP 13, 137 (1961)).R. A. Stradling and R. A. Wood,`
J. Phys. C1, 1711 (1968)
hlo = N hc
hc = eB/m*
1/BN hlo = N e/m*
Measurement of Effective Massas a Function of Temperature
Fermi Liquid behavior: excuse for BCS approach
A80[T]H
A181
)0(H2)0(
c
c
e
Hc2 and
AB
Modeling electron-phonon coupling in anthracene
extvibreeKEtotal HHHHH
vibrplaneinhoppingtotal HHH
after the LDA/Hartree calculation this reduces to
vibrtotal HccccrtH BAAB ),,,, ˆˆˆˆ(),(
RRRR
R,
††
0KE
H phonelecH
Su-Schrieffer-Heeger electron-phonon coupling
Ruu
ttrt m
mm
~~,
6
1 2,10 Assume crystal screening :
omission of the Holstein term