graphene: electrons in the flatland antonio h. castro neto
DESCRIPTION
Graphene: electrons in the flatland Antonio H. Castro Neto. Seoul, September 2008. Disclaimer. Andre Geim. Philip Kim. Kostya Novoselov. IQHE measured. Graphene is discovered. AHCN, P. Guinea, N. Peres, K. Novoselov, A. Geim, Rev. Mod. Phys. (2008). A brief history of graphene. 5 m m. - PowerPoint PPT PresentationTRANSCRIPT
Graphene: electrons in the flatland
Antonio H. Castro Neto
Seoul, September 2008
Disclaimer
Graphene is discovered
IQHE measuredAndre Geim
Kostya Novoselov
Philip Kim
AHCN, P. Guinea, N. Peres, K. Novoselov,A. Geim, Rev. Mod. Phys. (2008)
A brief history of graphene
5 m
Plus some nanotechnology…
2m
SiO2
Si
Au contacts
graphite
optical image
SEM imagedesign contacts and mesa
t ~ 2.7 eV
Some electronic properties of graphene
B
t’ ~ 0.1 eV
A
A
Unit cell Nearest neighborsNext Nearest neighbors
In momentum space
300/2
3
0 with ),(
)(
2242
22
cta
v
mpvvmmpE
pvppvpE
F
FF
FyxF
Dirac Cone
Semi-Metal
“Ultra relativistic” Solid State at low speed of light
Novoselov et al, Science 306, 666 (2004)
Outline•Coulomb impurity in graphene Vitor M. Pereira, Johan Nilsson, AHCN Phys.Rev.Lett. 99, 166802 (2007); Vitor M. Pereira, Valeri Kotov, AHCN Phys. Rev. B 78, 085101 (2008).
•Anderson impurity in graphene Bruno Uchoa, Valeri Kotov, Nuno Peres, AHCN Phys. Rev. Lett. 101, 026805 (2008);
Bruno Uchoa, Chiung-Yuan Lin, Nuno Peres, AHCN
Phys.Rev.B 77, 035420 (2008).
Johan Nilsson
Bruno Uchoa
Vitor Pereira
Valeri Kotov
Nuno Peres
Pereira et al., Phys.Rev.Lett. 99, 166802 (2007);
3D Schroedinger l
Coupling
UndercriticalSupercritical
Andrei’s group
HIC Neutron stars
LmvF
C
ar
a
t
aL
C
21
50
06.0
107
1 nm
E
N(E)
0
U0
Anderson’s Impurity Model
T>TK
00 00
Non-interacting: U=0
Broadening
EnergyEnergy
0
V=0
R
00
Mean-Field
00
The impurity moment can be switched on and off!
U = 1 eV
n_down
V=1eV, e0=0.2 eV
n_up
U = 40 meV
U = 0.1 eV
Conclusions
• Impurities in graphene behave in an unusual way when compared to normal metals and semiconductors.
• One can test theories of nuclear matter under extreme conditions.
• Control of the magnetic moment formation of transition metals using electric fields.