dirac fermions in graphite and graphene igor lukyanchuk amiens university i. lukyanchuk, y....
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Dirac fermions in Graphite and Graphene
Igor Lukyanchuk Amiens University
I. Lukyanchuk, Y. Kopelevich et al.
- Phys. Rev. Lett. 93, 166402 (2004)- Phys. Rev. Lett. 97, 256801 (2006)
Graphene2005
Novoselov, et al. Nature 438, 197 (2005
Y. Zhang, et al., Nature 438, 201 (2005
Why graphene is interesting ?
- Fundamental physics
- Applications (carbon-based microelectronics )
3D 2D 1D 0D
(Nobel prize) (Nobel prize)
2 view of Graphene
Nanotube-grapheneGraphite-graphene
“ “:
November 2005
• Graphene active area covering an entire 8-inch wafer• Carrier mobility of the FET exceeding 15,000 cm2/V-s• Drain voltage of the FET smaller than 0.25 V• ft and fmax both larger than 500 GHz• W-band low noise amplifier with >15 dB of gain and <1dB of noise figure• Wafer yield of the low noise amplifiers is more than 90%
30 000 000 $
HP, Intel, IBM…
Wanted:
Linear Dirac spectrum
Graphene: (2D graphite monolayer, Semimetal)
Special points of Brillouin zone
Brillouin zone 4-component (Dirac ????) wave function
"Normal electrons" “Dirac fermions"
Schrödinger equation Dirac equation
Dirac spinor
Free Relativistic Electrons
Gap formation, excitonic insulator, weak ferromagnetism, … ???
Abrikosov Phys. Rev. B60, 4231 (1999) B61, 5928 (2000)
Khveshchenko, Phys. Rev. Lett. 87, 206401 (2001); 87, 246802 (2001)
González, Guinea, Vozmediano, Phys. Rev. Lett. 77, 3589 (1996)
In magnetic field: 2 component equations
Schroedinger cond-mat physics
Dirac cond-mat physics !!!
Klein effect:
U(x)
U(x)
Ef
Ef
electron
electron
holehole
Metal (semiconductor)
Semimetal:
No electron localization !!!
Minimal conductivity
Band structure: Slonczewski-McClure Model
Graphite:F
ittin
g pa
ram
eter
s
holes
electrons
ρ(T), HOPG
In best samples
ρc/ ρa > 50000 (instead of 300 in Kish)
ρa ~ 3 μΩ cm (300K)
n3D~3x1018 cm-3
n2D~1011 cm-2 (1012-1013 in Graphene)
Mobility:
μ~106cm2/Vs (104 in Graphene)
Metals: 300μΩ cm, Ioffe-Regel 1000 μΩ cm
Novoselov, K. S. et al. Nature 438, 197 (2005); Zhang, Y. et al. Nature 438, 201 (2005).
2005: Discovery of Quantum Hall Effect in 2D Graphene Due to Dirac fermions …
From: - phase analysis - semi-integerr QHE
Quantum Hall Effect, different samples (2003)
0 1 2 3 4 50
1
2
3
4
5
Filling Factor
-
Gx
y /
G0
xy
Normal QHE
-8
-4
0
4
8
-
Rx
x
( m
)
0 1 2 3 4 5 6 7 80
1
2
3
4
5
6
7
8
9
-
Gxy
/G0
xy
B0/B
HOPG, Y. Kopelevich et al. PRL´2003
Few Layer Graphite (FLG)K.S.Novoselov et al., Science´2004
B0= 20 T, = > n ~ 2x1012cm-2
B0 = 4.68 T
Fig. 1
1
2
B0 = 4.68 T
Few Layer Graphite (FLG)K.S.Novoselov et al., Science´2004
B0= 20 T, = > n ~ 2x1012 cm-2
.
QHE: Graphite vs multi graphene
HOPG, Y. Kopelevich et al. PRL´2003
Do Dirac Fermions Exist in Graphite ?
Normal electrons
Dirac electrons
Landau quantization: Normal vs Dirac
‘’gap’’
no ‘’gap’’ !!!
SdH: Oscillations of xx (H) (1st harmonic)
Normal: = 1/2Dirac: = 0► Spectrum : {
2D: = 03D: = ± 1/8► Dimensionality :{
Phase depends on :
dHvA: Oscillations of (H) (1st harmonic)
Cyclotron mass(detection of e and h)
SdHdHvA
Experiment:
Electrons or Holes ?
Normal or Dirac ?
SdH dHvA
dHvASdH
Pass-band filtering
spectrum
Comparison of dHvA and SdH
electrons
holes
In-phase
Out-phase
Fan Diagram for SdH oscillations in Graphite
Dirac
Normal
Novoselov, 2005
graphene
Multilayer 5nm graphite
holes
electrons
Dirac Spectrum
Normal Spectrum
H: point
Phase volume ~0
no Dirac Fermionsshould be seen in experiment
Problems with band interpretation
Se > Sh1)
2)
Sh > Se
Independent layers ???
Another possibility:
2006 Confirmation: Angle Resolved Photoemission Spectroscopy
Dirac holes
Normalelectrons
(ARPES)
E. Andrei et al. 2007, Nature Phys.
Dirac+Normal fermions in HOPGTEM results:
Another confirmation of Dirac fermions:
Interlayer tunneling spectroscopy of Landau levels in graphiteYu. I. Latyshev1, A. P. Orlov1, V. A. Volkov1, A. V. Irzhak2, D. Vignolles3, J. Marcus4 and T. Fournier4
0 1 2 3 4 5 6-400
-300
-200
-100
0
100
200
300
400
Mag.trans 2x(01) STM 2x(01) STM 2x(02) Inter.tunn -11 Inter.tunn -22 Inter.tunn -33
V (
mV
)
B (T)
Graphite #1
OPTICAL PROPERTIES
- Visible- Infrared- Raman
Graphite
Graphene
C=
Reflectance and transmitance coefficients
Optical properties are defined by HF conductivity
πα ≈ 2.3%
INFRARED SPECTROSCOPY
nE)n(sign
nBe2v)n(signE
10
Fn
2006
Graphite, interpretation, ??? =>
RAMAN SPECTROSCOPY
RAMAN SPECTROSCOPY
« Graphene Fingerprint »
E =
2.3
3 e
V
0.4 0 0.20.400.2-2
-1
0
1
2
E (
eV
)
KK MM M
q’
q
q’’A
B C
double-resonant
0 1500 3000Raman shift (cm-1)
Inte
nsity
(a.
u) graphite 2.33 eV
D
G
D‘ G‘
Raman spectra of graphite
HOPG, Raman
model