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An introduction to the theory of Carbon nanotubes
A. De Martino
Institut für Theoretische Physik
Heinrich-Heine Universität
Düsseldorf, Germany
Overview
Introduction
Band structure and electronic properties
Low-energy effective theory for SWNTs
Luttinger liquid physics in SWNTs
Experimental evidence
Summary and conclusions
Allotropic forms of Carbon
Curl, Kroto, Smalley 1985
Iijima 1991graphene
(From R. Smalley´s web image gallery)
Classification of CNs:single layer
Single-wall Carbon nanotubes (SWNTs,1993)- one graphite sheet seamlessly wrapped-up to form a cylinder
- typical radius 1nm, length up to mm
(From R. Smalley´s web image gallery)
(From Dresselhaus et al., Physics World 1998)
(10,10) tube
Classification of CNs: ropes
Ropes: bundles of SWNTs- triangular array of individual SWNTs
- ten to several hundreds tubes
- typically, in a rope tubes of different diameters and chiralities
(From R. Smalley´s web image gallery)(From Delaney et al., Science 1998)
Classification of CNs: many layers
Multiwall nanotubes (Iijima 1991)
- russian doll structure, several inner shells
- typical radius of outermost shell > 10 nm
(From Iijima, Nature 1991) (Copyright: A. Rochefort, Nano-CERCA, Univ. Montreal)
Why Carbon nanotubes so interesting ?
Technological applications- conductive and high-strength composites
- energy storage and conversion devices
- sensors, field emission displays
- nanometer-sized molecular electronic devices
Basic research: most phenomena of mesoscopic physics observed in CNs- ballistic, diffusive and localized regimes in transport
- disorder-related effects in MWNTs
- strong interaction effects in SWNTs: Luttinger liquid
- Coulomb blockade and Kondo physics
- spin transport
- superconductivity
Band structure of graphene
Tight-binding model on hexagonal lattice
- two atoms in unit cell
- hexagonal Brillouin zone
(Wallace PR 1947)
iRRBRA
cHcctHi
,,,0 ..
nm 0.142d ; nm 246.0a
eV37.2
t1
23
K K
Band structure of graphene
Tight-binding model- valence and conduction bands touch at E=0
- at half-filling Fermi energy is zero (particle-hole symmetry): no Fermi surface, six isolated points, only two inequivalent
Near Fermi points
relativistic dispersion relation
Graphene: zero gap semiconductor
m/s108,
,5
FF
F
vKkq
qvqE
(Wallace PR 1947)
Structure of SWNTs: folding graphene
(n,m) nanotube specified by wrapping, i.e. superlattice vector:
Tube axis direction
21 amanC
2211 aatT
)2,2gcd(
/)2(
/)2(
2
1
nmmnd
dmnt
dnmt
R
R
R
Structure of SWNTs
(n,n)
armchair
(n,0)
zig-zag
chiral
(4,0)
Electronic structure of SWNTs
Periodic boundary conditions → quantization of
- nanotube metallic if Fermi points allowed wave vectors,
otherwise semiconducting !
- necessary condition: (2n+m)/3 = integer
k
armchair zigzag
metallic semiconducting
Electronic structure of SWNTs
Band structure predicts three types:
- semiconductor if (2n+m)/3 not integer; band gap:
- metal if n=m (armchair nanotubes)
- small-gap semiconductor otherwise (curvature-induced gap)
Experimentally observed: STM map plus conductance measurement on same SWNT
In practice intrinsic doping, Fermi energy typically 0.2 to 0.5 eV
eV13
2
R
vE F
Density of states
Metallic tube:
- constant DoS around E=0
- van Hove singularities at opening of new subbands
Semiconducting tube:
- gap around E=0
Energy scale ~1 eV
- effective field theories valid for all relevant temperatures
Metallic SWNTs: 1D dispersion relation
Only subband with relevant, all others more than 1 eV away
- two degenerate Bloch waves, one
for each Fermi point α=+/-
- two sublattices p =+/-, equivalent
to right/left movers r =+/-
- electron states
- typically doped:
0k
r
KkvEq FFFF
/
SWNTs as ideal quantum wires
Only one subband contributes to transport
→ two spin-degenerate channels
Long mean free paths
→ ballistic transport in not too long tubes
No Peierls instability
SWNTs remain conducting at very low temperatures → model systems to study correlations in 1D metals
m1
Conductance of ballistic SWNTs
Landauer formula: for good contact to voltage reservoirs, conductance is
Experimentally (almost) reached- clear signature of ballistic transport
What about interactions?
h
e
h
eNG bands
22 42
Including electron-electron interactions in 1D
In 1D metals dramatic effect of electron-electron interactions: breakdown of Landau´s Fermi liquid theory
New universality class: Tomonaga-Luttinger liquid
- Landau quasiparticles unstable excitations
- stable excitations: bosonic collective charge and spin density fluctuations
- power-law behaviour of correlations with interaction dependent exponents → suppression of tunneling DoS
- spin-charge separation; fractional charge and statistics
- exactly solvable by bosonization
Experimental realizations: semiconductor quantum wires, FQHE edges states, long organic chain molecules, nanotubes, ...
(Tomonaga 1950, Luttinger 1963, Haldane 1981)
Luttinger liquid properties
1d electron system with dominant long-range interaction
- charge and spin plasmon densities; - spin-charge separation !
- depends on interaction :
Suppression of tunnelling density of states at Fermi surface :
- exponent depends on geometry (bulk or edge)
ExtxedtEx iEt
)0,(),(Re1
),(0
22222LL 22 sxs
Fcxcc
F dxv
Kdxv
H
sxcx ,
cK1
1
c
c
K
K no interaction
repulsive interaction
Field theory of SWNTs
Low-energy expansion of electron field operator:
- Two degenerate Bloch states
at each Fermi point
Keep only the two bands at Fermi energy,
Inserting expansion in free Hamiltonian gives
)()()( ''0 xxdxivH pppxxpF
1
0;
0
1
2,
BA
p
rKi
pR
eyx
p
pp yxFyxyx ),(,,
(Egger and Gogolin PRL1997, Kane et al. PRL 1997)
0k
)(),( xyxF pp
Coulomb interaction
Second-quantized interaction part:
Unscreened potential on tube surface
2222
2
2
´sin4´)(
/
zaR
yyRxx
eU
rrrrUrrrdrdH I
´´´´
2
1´´
´
1D fermion interactions
Momentum conservation allows only two type of processes away from half-filling
- Forward scattering: electrons remain at same Fermi point, probes long-range part of interaction
- Backscattering: electrons scattered to opposite Fermi point, probes short-range properties of interaction
- Backscattering couplings scale as 1/R, sizeable only for ultrathin tubes
Backscattering couplings
Fk2
Momentum exchange
Fq2
Coupling constant
Reaf /05.0/ 2Reab /1.0/ 2
Bosonization:
four bosonic fields (linear combinations of )- charge (c) and spin (s)
- symmetric/antisymmetric K point combinations
Bosonized Hamiltonian
Effective low-energy Hamiltonian
termsnonlinear2
222 aaaa
F Kv
dxH
),,,( ssccaa
(Egger and Gogolin PRL1997, Kane et al. PRL 1997)
rFF ixirqxki
r e 4~
r
Luttinger parameters for SWNTs
Bosonization gives
Long-range part of interaction only affects total charge mode
- logarithmic divergence for unscreened interaction, cut off by tube length
very strong correlations !
3.02.02ln8
12/12
RL
v
eKg
Fc
1caK
Phase diagram (quasi long range order)
Effective field theory can be solved in practically exact way
Low temperature phases matter only for ultrathin tubes or in sub-mKelvin regime
bF RRbvbB
bf
eDeTk
TbfT//
)/(
Theoretical predictions
Suppression of tunneling DoS:
- geometry dependent exponent:
Linear conductance across an impurity:
Universal scaling of scaled non-linear conductance across an impurity as function of
EEx ),(
4/)1/1(
8/2/1
g
gg
end
bulk
endTTG 2)(
TkeV B/
Evidence for Luttinger liquid
(Yao et al., Nature 1999)
gives 22.0g
end2
bulk
Conclusions
Effective field theory + bosonization for low-energy properties of SWNTs
Very low-temperature : strong-coupling phases
High-temperature : Luttinger liquid physics
Clear experimental evidence from tunnelling conductance experiments