Fundamental physics with two-dimensional carbon
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Transcript of Fundamental physics with two-dimensional carbon
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Fundamental physics with two-dimensional carbon
Igor Herbut (Simon Fraser University, Vancouver)
Chi-Ken Lu (Indiana)Bitan Roy (Maryland) Vladimir Juricic (Utrecht)Oskar Vafek (Florida)Gordon Semenoff (UBC)Fakher Assaad (Wurzburg)Vieri Mastropietro (Milan)
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Two triangular sublattices: A and B; one electron per site (half filling)
Tight-binding model ( t = 2.5 eV ):
(Wallace, PR 1947)
The sum is complex => two equations for two variables for zero energy
=> Dirac points (no Fermi surface)
Single layer of graphite: graphene (Geim and Novoselov, 2004)
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Brillouin zone:
Two inequivalent (Dirac) points at :
+K and -K
Dirac fermion: 4 components/spin component
“Low - energy” Hamiltonian: i=1,2
,
(isotropic, v = c/300 = 1, in our units). Neutrino-like in 2D!
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1) Cone’s isotropy (rotational symmetry); Lorentz invariance!
2) Chiral (valley, or pseudospin):
=
,
3) Time reversal (exact)
4) Spin rotational invariance (exact)
Symmetry: emergent and exact
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Does not Coulomb repulsion matter: yes, but!
with the interaction term, (Hubbard + Coulomb)
Long-range part is not screened, and it may matter.
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The Fermi velocity depends on the scale: (Gonzalez et al, NPB 1993)
To the leading order:
and the Fermi velocity increases! It goes to where
which is at the velocity (in units of velocity of light):
= >
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The ultimate low-energy theory: reduced QED3 (matter in 2+1 D + gauge fields in 3+1 D)Gauge field propagator:
and the fine structure constant is scale invariant!! Dirac fermions are massless, with a velocity of light.
Experiment: (Ellias et al, Nature 2011)
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Back to reality: should we not worry about finite-range pieces of Coulomb interaction? Yes, in principle:
(Grushin et al, PRB 2012) (IH, PRL 2006)
At large interaction some symmetry gets broken.
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Masses (symmetry breaking order parameters):
1) “Charge-density-wave” (Semenoff, PRL 1984 (CDW); IH, PRL 2006 (SDW))
2) Kekule bond-density-wave(Hou, Chamon, Mudry, PRL 2007)
Chiral triplet, Lorentz singlets, time-reversal invariant!
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3) Topological insulator (Haldane, PRL 1988)
Lorentz and chiral singlet, breaks time-reversal.
4) + all these in spin triplet versions (+ 4 superconducting states)
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Gross-Neveu-Yukawa theory: epsilon-expansion, epsilon = 3-d (IH, Juricic, Vafek, PRB 2009)
Field theory: (for SDW transition, only)
Neel order parameter: (Higgs field)
With Coulomb long-range interaction:
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RG flow, leading order:
CDW (SDW)
Exponents:
Long-range “charge”:
and marginally irrelevant !
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Emergent relativity: if we define a small deviation of velocity
it is (the leading) irrelevant perturbation close to d=3 :
and of bosonic and fermionic masses.
Transition: from gapless (fermions) to gapless (bosons)!
Consequence: universal ratio of specific heats
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Finite size scaling in quantum Monte Carlo:
near d=3,
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Uc = 3.78
Crossing point and the critical interaction (from magnetization)
This suggests: (in Hubbard)
(F. Assaad and IH, PRX 2013)
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Anything at low U?? Meet the artificial graphene: (Gomes, 2012)
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Hubbard model with a flat band: (Roy, Assaad, IH, PRX 2014)
“Global antiferromagnet”
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Back to Dirac masses: SO(5) symmetry
An example:
(SDW (3 masses), Kekule (2 masses))
These 5 masses and the 2 (alpha) matrices in the Dirac Hamiltonian form a maximal anticommuting set of dimension 8: Clifford algebra
C(2,5)This remains true even if all the possible superconducting masses are included: (Ryu et al, PRB 2010)
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To include superconducting masses Nambu doubling is necessary: matrices become 16x16, but (antilinear!) particle-hole symmetry restricts:
1) Masses to be purely imaginary
2) Alpha matrices to be purely real
This separation leads to C(2,5) as the maximal algebra.
16x16 representation, however, is “quaternionic”:
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Real representations of C(p,q): (IH, PRB 2012, Okubo, JMP 1991, ABS 1964)
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Example: U(1) superconducting vortex (s-wave, singlet) (IH, PRL 2010)
: {CDW, Kekule BDW1, Kekule BDW2}
: {Haldane-Kane-Mele TI (triplet)}
Lattice: 2K componentExternal staggered potential
Core is insulating ! (Ghaemi, Ryu, Lee, PRB 2010)
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Conclusions:
1) Honeycomb lattice: playground for interacting electrons
2) Coulomb interaction: 1) long ranged, not screened, but ultimately innocuous, 2) short range leads to symmetry breaking
3) Novel (Higgs) quantum phase transition in the Hubbard model; global antiferromagnet under strain
4) SO(5) symmetry of the Dirac masses (order parameters) implies duality relations and non-trivial topological defects