aspects of the spinon fermi-surface state max metlitski
TRANSCRIPT
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Aspects of the spinon Fermi-surface state
Max Metlitski
Kavli Institute for Theoretical Physics
KITP Workshop on Frustrated Magnetism and Quantum Spin
Liquids, October 3, 2012
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Plan:
• Introduction to the spinon Fermi-surface state of U(1) spin-liquid and some
motivation
• Relation to
- Quantum Hall effect at ν = 1/2
- Phase transitions in metals
• Theoretical status of the problem
• BCS pairing of the spinon Fermi-surface state
- transition from a U(1) → Z2 spin-liquid
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Spin-liquids
• “Exotic” Mott insulators
with no symmetry breaking.
• Fractionalize
• fermionic quasiparticles (spinons)
See e.g. Arun Paramekanti’s talk
or review by P.A.Lee, N. Nagaosa and X.G. Wen, RMP (2006)
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Spinon Fermi-surface
• Imagine is such that the spinons form a Fermi-surface
- lots of low energy spin excitations
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Weak Mott Insulator
• Evidence that this situation occurs on a triangular lattice
AFM Spin-liquid Metal
H. Morita, S. Watanabe and M. Imada (2002)
H.-Y. Yang, A. M. Lauchli, F. Mila, and K. P. Schmidt (2010)
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Slave-boson theory
• A natural path to this phase diagram – slave boson (rotor) representation
• - bosonic rotor variable
- fermionic spinon
AFM Spin-liquid Metal
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Slave-boson theory
Spin-liquid Metal
charge – gapped
spin - gapless
• Some numerical evidence for spinon FS in the spin liquid state on triangular lattice
H.-Y. Yang, A. M. Lauchli, F. Mila, and K. P. Schmidt (2010)
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Material!!
• Experimental candidate: organic triangular lattice insulator EtMe3Sb[Pd(dmit)2]2
M. Yamashita et. al., (2011)S. Yamashita et. al., (2011)
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Material!!
• Experimental candidate: organic triangular lattice insulator EtMe3Sb[Pd(dmit)2]2
• Low energy properties like a Fermi-liquid (except an insulator)!
• But are these actually properties of the spinon FS state?
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Effective theory of spinon Fermi-surface state
•
• Invariant under a local symmetry
• Low energy description will involve a compact U(1) gauge field
• Note: the spinon representation actually has a larger SU(2) symmetry
However, the mean-field Hamiltonian
breaks .
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Effective theory of spinon Fermi-surface state
• Low energy theory involves gapless spinons near the Fermi-surface and gapless
fluctuations of the U(1) gauge field.
• The coupling of gauge-fluctuations to spinons destroys sharp spinon
quasiparticles.
• Non-Fermi-liquid (critical Fermi-surface) of spinons.
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Plan:
• Introduction to the spinon Fermi-surface state of U(1) spin-liquid and some
motivation
• Relation to
- Quantum Hall effect at ν = 1/2
- Phase transitions in metals
• Theoretical status of the problem
• BCS pairing of the spinon Fermi-surface state
- transition from a U(1) → Z2 spin-liquid
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Half-filled Landau level
R. Willet et. al. (87)
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Half-filled Landau level: Composite Fermion Liquid
• Form composite fermions by attaching two flux-quanta to each electron
• Composite fermions see no net magnetic field and form a Fermi-surface
• A U(1) Chern-Simons gauge field is used to attach flux:
• Fluctuations of make the Fermi-surface of the composite fermion critical.
B. I. Halperin, P. A. Lee, N. Read (1993)
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Half-filled Landau level
• Fractional QH states near
can be interpreted as Integer QH
states of the composite fermion
liquid.
• Strong experimental evidence
for emergence of a Fermi-surface
at (e.g. from surface-
acoustic wave).
• Strong numerical evidence for
emergence of Fermi-surface.
• Conflicting results regarding criticality of the Fermi-surface.
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Phase transitions in metals
Fermi liquid
• Order parameter:
Non-Fermi-
liquid
Fermi liquid
• heavy-fermion compounds, Sr3Ru2O7, electron-doped cuprates, pnictides,
organics, hole-doped cuprates
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Critical Fermi surface states
• Spinon Fermi-surface state of Mott-insulators
(Bose metals)
• Composite-fermion liquid of QHE system
• Phase transitions in metals
• All three states involve a Fermi surface interacting with a gapless boson
• Difficult problem, due in part to an absence of a full RG program.
• “Solved” in limit in early 90’s
Declared open again after work of S. S. Lee (2009).
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Plan:
• Introduction to the spinon Fermi-surface state of U(1) spin-liquid and some
motivation
• Relation to
- Quantum Hall effect at ν = 1/2
- Phase transitions in metals
• Theoretical status of the problem (focus on dimension d = 2)
• BCS pairing of the spinon Fermi-surface state
- transition from a U(1) → Z2 spin-liquid
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Emergence of gauge field
• - local Lagrange multiplier enforcing the single occupancy constraint.
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Emergence of gauge field
• - Hubbard-Stratonovitch field.
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Emergence of gauge field
• Focus on slow fluctuations .
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Theory of the spinon Fermi-surface
• Theory of a gapless gauge field interacting with the spinon Fermi-surface
• Integrate the fermions out at the RPA level (work in gauge):
• Magnetic field fluctuations are very soft:
- Debye screened
- Landau damped
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Feedback on the fermions
• Non Fermi-liquid!
P. A. Lee, N. Nagaosa (1992); J. Polchinski (1993);
B. I. Halperin, P. A. Lee, N. Read (1993).
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How to scale?
Gauge field: Fermions:
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• Most singular kinematic regime: two-patch
Two-patch regime
J. Polchinski (1993); B. Altshuler, L. Ioffe, A. Millis (1994).
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Why two-patch regime?
• Cannot effectively absorb a Landau-damped bosonic mode.
• Gauge fluctuations are very soft:
B. Altshuler, L. Ioffe, A. Millis (1994).
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Why two-patch regime?
• This “conspiracy” between fermions and bosons is special to 2+1 dimensions.
• Gauge fluctuations are very soft:
B. Altshuler, L. Ioffe, A. Millis (1994).
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• For each expand the fermion fields about two
opposite points on the Fermi surface, and .
• Crucial to keep the Fermi-surface curvature radius finite.
Two-patch theory
J. Polchinski (1993); S. S. Lee (2009)
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• Have a large set of 2+1 dimensional theories
labeled by points on the Fermi-surface ( )
• Key assumption: can neglect coupling between patches.
Two-patch theory
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Anisotropic scaling
• Fermion kinetic term dictates:
• A symmetry of the theory guarantees that this scaling is exact.
J. Polchinski (1993); B. Altshuler, L. Ioffe, A. Millis (1994).
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Two-patch scaling
Critical Fermi surface Fermi-liquid
does not flow
J. Polchinski (1993); B. Altshuler, L. Ioffe, A. Millis (1994), S. S. Lee (2008).
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Scaling properties
• Reproduces RPA at one loop
• Theory strongly coupled
• Symmetries constrain the RG properties severely
• Only two anomalous dimensions
- fermion anomalous dimension
- dynamical critical exponent
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Scaling forms: gauge field
•
• Simple Landau-damped frequency dependence consistent with scaling form
• Static behaviour
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Scaling forms: fermions
•
• “Fermionic dynamical exponent” is half the “bosonic dynamical exponent”
• Static behaviour:
• Dynamic behaviour:
• ``Tunneling density of states”:
M.M and S. Sachdev (2010)
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Problem
• No expansion parameter. Theory strongly coupled.
• Direct large- expansion fails.
• A more sophisticated genus expansion also fails. Unknown if
limit exists.
• Uncontrolled three loop calculations
S. S. Lee (2009)
M.M. and S. Sachdev (2010)
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Problem
• Uncontrolled three loop calculations give
• Contrary to the previous belief that no qualitatively new physics beyond one
loop.
M.M. and S. Sachdev (2010)
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How to control the expansion?
• Long-range interaction in the half-filled Landau level
• - Coulomb interaction
- contact interaction
B. I. Halperin, P. A. Lee, N. Read (1993); C. Nayak and F. Wilczek (1994)
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How to control the expansion?
• Perform more conventional scaling dictated by the fermion kinetic term:
• Fermion-gauge field interactions are at tree level:
• Theory described by a single dimensionless coupling constant:
- irrelevant
- relevant
- marginal
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ε-expansion
• Quantum corrections to scaling
C. Nayak and F. Wilczek (1994)
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•
- interactions marginally irrelevant.
“Marginal Fermi-liquid.”
ε-expansion
C. Nayak and F. Wilczek (1994)
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•
- new fixed-point:
ε-expansion
C. Nayak and F. Wilczek (1994)
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Beyond one-loop
• Two expansions have been suggested:
potential difficulty:
systematic counting of powers of needs to be done!
cannot be applied to the case.
- - fixed, “perturbative” expansion
C. Nayak and F. Wilczek (1994)
- - fixed, - expansion.
D. Mross, J. McGreevy, H. Liu and T. Senthil (2010)
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Response functions
• Same as before,
• Except non-locality of the action constrains
• at three loop order.
D. Mross, J. McGreevy, H. Liu and T. Senthil (2010)
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Open questions
• Prove (disprove) that in physical theory
- for dMIT
• Systematic theory of forward-scattering channel
- holds for dMIT
• Transport properties
• Monopole effects
C.P.Nave, S.S.Lee and P.A.Lee (2006)
C.P.Nave and P.A.Lee (2007)
- monopoles irrelevant (confined)L.B.Ioffe and A.I.Larkin (1989),
S.S.Lee (2008)
- for dMIT
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Plan:
• Introduction to the spinon Fermi-surface state of U(1) spin-liquid and some
motivation
• Relation to
- Quantum Hall effect at ν = 1/2
- Phase transitions in metals
• Theoretical status of the problem
• BCS pairing of the spinon Fermi-surface state
- transition from a U(1) → Z2 spin-liquid
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Collaborators
Subir Sachdev Senthil Todadri David Mross
(Harvard) (MIT) (MIT)
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• A regular Fermi-liquid is unstable to arbitrarily weak attraction in the
BCS channel.
• How about the spinon Fermi-surface?
Pairing of critical Fermi surfaces
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• Magnetic fluctuations mediate a long-range repulsion
• Can a short range attractive interaction compete with this?
• What is the critical interaction strength?
Pairing instability of spinon Fermi-surface
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Pairing in a spin-liquid
U(1) spin-liquid
spinon Fermi surface- spin-liquid
Excitations: gapless spinons
gapless gauge (magnetic field)
fluctuations
gapped spinons
gapped Abrikosov vortices
(visons)
• Previous theoretical work claims a fluctuation induced first order transition
M. U. Ubbens and P. A. Lee (1994)
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• Attraction for spinons on same side of the Fermi-surface
• Sympathetic to LOFF-like pairing
• Not discussing this possibility. For , system is “far” from this instability.
Amperean pairing
Sung-Sik Lee, Patrick A. Lee, T. Senthil (2007)
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• Scattering amplitude in the BCS channel at
• In the regime , the one loop diagram is enhanced by
•
irrelevant in two-patch theory marginal in Fermi-liquid theory
Pairing singularities
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• Low-energy states on the Fermi-surface cannot be integrated out
Conceptual difficulties with two-patch RG
•
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• Treatment of the pairing instability requires a marriage of two RG’s:
Conceptual difficulties with two-patch RG
does not flow
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Son’s RG procedure
• Keep interpatch couplings!
D. T. Son, Phys. Rev. D 59, 094019 (1999).
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Perturbations
• Only two types of momentum conserving processes keep fermions on the FS
Forward-scattering BCS scattering
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Fermi-liquid RG
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Son’s RG
• Generation of inter-patch couplings:
• Generates an RG flow:
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Combined RG
- (from intra-patch theory)
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Pairing of the spinon Fermi-surface
• Need a finite attraction to drive the pairing instability.
• Gap onsets as
Spinon FSPairing
transition
M.M., D. Mross, S. Sachdev, T. Senthil, forthcoming
- spin-liquid
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• All results for can be reproduced by summing rainbow graphs in
the Eliashberg approximation.
Eliashberg approximation
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Properties of the paired state near transition
- is the “superconductor” type I or type II close to the transiton?
Likely type I:
- Motrunich effect
- Abrikosov lattice of visons unstable.
- how does the vortex mass (vison gap) vanish at the pairing transition?
Spinon FSPairing
transition- spin-liquid
O.I.Motrunich (2006)
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Conclusion
• Progress (and new challenges) in understanding spinon Fermi-surface state
and its relatives.
• First theory of pairing transition out of the spinon Fermi-surface state.
• Lots of open questions
Thank you!