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Vladimir Cvetković
Physics Department ColloquiumColorado School of Mines
Golden, CO, October 2, 2012
Electronic MulticriticalityIn Bilayer Graphene
National High Magnetic Field LaboratoryFlorida State University
National High Magnetic Field Laboratory
Superconductivityhttp://www.magnet.fsu.edu/mediacenter/seminars/winterschool2013/
Collaborators
Dr. Robert E. Throckmorton Prof. Oskar Vafek
V. Cvetkovic, R. Throckmorton, O.Vafek, Phys. Rev. B 86, 075467 (2012)
NSF Career Grant (O. Vafek): DMR-0955561
Graphite
Carbon allotrope
Greek (γράφω) to write
Graphite: a soft, crystalline form of carbon. It is gray to black, opaque, and has a metallic luster. Graphite occurs naturally in metamorphic rocks such as marble, schist, and gneiss.
U.S. Geological Survey
Mohs scale 1-2
Graphite electronic orbitals
Orbitals:• sp2 hybridization (in-plane bonds)• pz (layer bonding)
Hexagonal lattice• space group P63/mmc
Massless Dirac fermions in graphene
bond
Strong cohesion (useful mechanical properties)
bond
Interesting electronic properties
Massless Dirac fermions in graphene
Sufficient conditions: C3v and Time reversalNecessary conditions: Inversion and Time reversal(*if Spin orbit coupling is ignored)
Dirac cones:
Tight binding Hamiltonian
where
Spectrum
Velocity: vF = t a ~106 m/s
Graphene fabrication
Obstacle: Mermin-Wagner theoremFluctuations disrupt long range crystalline order in 2D at any finite temperature
Epitaxially grown graphene on metal substrates (1970):Hybridization between pz and substrate
Exfoliation: chemical and mechanical
Scotch Tape method (Geim, Novoselov, 2004)
YouTube Graphene Making tutorial (Ozyilmaz' Group)
How to see a single atom layer?
Si
SiO2300nm
graphene
P. Blake, et al, Appl. Phys. Lett. 91, 063124 (2007)
Ambipolar effect in Graphene
A. K. Geim & K. S. Novoselov, Nature Materials 6, 183 (2007)
Isd
Vg
Graphene
Mobility:• = 5,000 cm2/Vs (SiO2 substrate, this sample = 2007)• = 30,000 cm2/Vs (SiO2 substrate, current)• = 230,000 cm2/Vs (suspended)
Graphene in perpendicular magnetic field: QHE
Isd
Vg
Graphene
H
Hall bar geometry
IQHE: Novoselov et al, Nature 2005Room temperature IQHE: Novoselov et al, Science 2007
Graphene in perpendicular magnetic field: FQHE
FQHE: C.R. Dean et al, Nature Physics 7, 693 (2011)
Bilayer Graphene
Two layers of grapheneBernal stacking
K K'
t
3t
t
3t
Ek
Tight binding Hamiltonian
Spectrum
Trigonal warping inBilayer Graphene
Parabolic touching is fine tuned (3 = 0)
2:4meV1:6meV
0:8meV
Tight binding Hamiltonian with 3 :
Vorticity:
Bilayer Graphene in perpendicular magnetic field
Isd
Vg
BLG
H
Hall bar geometry
IQHE: Novoselov et al, Nature Physics 2, 177 (2006)
Widely tunable gap inBilayer Graphene
Y. Zhang et al, Nature 459, 820 (2009)
Trilayer Graphene
ABA and ABC stacking
Band structureABC Trilayer Graphene
Tight binding Hamiltonian
Non-interacting phases inABC Trilayer Graphene
Phase transitions, even with no interactions
Spectrum:
3+9-3-
c2 c1
Electron interactions(Mean Field)
An example: Bardeen-Cooper-Schrieffer Hamiltonian (one band, short range)
Superconducting order parameter
Decouple the interaction into quadratic part and neglect fluctuations
The transition temperature
Debye frequency D = 2/2m Only when g>0 !
0
Different theories at different scales (RG)
What if D were different? Make a small change in :
How to keep Tc the same?
This example shows that the interaction is different at different scales.
The main idea of the renormalization group (RG):• select certain degrees of freedom (e.g., high energy modes, high momenta
modes, internal degrees of freedom in a block of spins...)• treat them as a perturbation• the remaining degrees of freedom are described by the same theory,
but the parameters (couplings, masses, etc) are changed
Our example (BCS): treat high momentum modes perturbatively (one-loop RG)
... but RG is much more powerful and versatile than what is shown here.
Finite temperature RG
Revisit our example (BCS)
Treat fast modes perturbatively
The change in the coupling constant
The effective temperature also changes
In this simple example we can solve the -function
... and find the Tc
Electron Interactions inSingle Layer Graphene
Rich and open problem, nevertheless in zero magnetic field:
Short-range interactions: irrelevant (in the RG sense) when weak.As a consequence, the perturbation theory about the non-interacting state becomes increasingly more accurate at
energies near the Dirac point
Coulomb interactions: marginally irrelevant (in the RG sense) when weak
semimetal* insulatorQCP
O. Vafek, M.J. Case, Phys. Rev. B 77, 033410 (2008)
In either case, a critical strength of e-e interaction must be exceeded for a phase transition into a different phase to occur. Hence, this is strong coupling problem.
Electron Interactions inBilayer Graphene
Short range interactions: marginal by power counting
Classified according to IR’s of D3d
The kinetic part of the action
where
Fierz identities implemented
Symmetry allowed Dirac bilinears (order parameters) in BLG
VC, R.E. Throckmorton, O. Vafek, Phys. Rev. B 86, 075467 (2012)
RG in BilayerGraphene (no spin)
Fierz identities reduce no of independent couplings to 4
O. Vafek, K. Yang, Phys. Rev. B 81, 041401(R) (2010)O. Vafek, Phys. Rev. B 82, 205106 (2010)
Susceptibilities (leading instabilities, all orders tracked simultaneously)
Possible leading instabilities: nematic, quantum anomalous Hall, layer-polarized, Kekule current, superconducting
Experiments on Bilayer Graphene
A.S. Mayorov, et al, Science 333, 860 (2011)
2:4meV1:6meV
0:8meV
Low-energy spectrum reconstruction
RG in Bilayer Graphene (spin-1/2)
Finite temperature RG with trigonal warping
VC, R.E. Throckmorton, O. Vafek, Phys. Rev. B 86, 075467 (2012)
Susceptibilities (determine leading instabilities)
… used to be tanh(1/2t)
Forward scattering phase diagram in BLG
Only
General phase diagram(density-density interaction)
Density-density interaction
Bare couplings in RG:
Coupling constantsfixed ratios
In the limitthe ratios of g’s are fixed
The leading instability depends on the ratios (stable ray)
Stable flows:• Target plane
• Ferromagnet• Quantum anomalous Hall• Loop current state• Electronic density instability
(phase segregation)
RG in Trilayer Graphene
Belongs to a different symmetry class
Number of independent coupling constants in Hint: 15
Spectrum
RG flow
Generic Phase Diagramin Trilayer Graphene
Trilayer Graphene(special interaction cases)
Forward scatteringHubbard model(on-site interaction)
Generic Phase Diagramin Trilayer Graphene