233 research outputs found
Symmetry and duality in bosonization of two-dimensional Dirac fermions
Recent work on a family of boson-fermion mappings has emphasized the
interplay of symmetry and duality: Phases related by a particle-vortex duality
of bosons (fermions) are related by time-reversal symmetry in their fermionic
(bosonic) formulation. We present exact mappings for a number of concrete
models that make this property explicit on the operator level. We illustrate
the approach with one- and two-dimensional quantum Ising models, and then
similarly explore the duality web of complex bosons and Dirac fermions in (2+1)
dimensions.Comment: 31 pages, 9 figure
Bosonic Analogue of Dirac Composite Fermi Liquid
We introduce a particle-hole-symmetric metallic state of bosons in a magnetic
field at odd-integer filling. This state hosts composite fermions whose energy
dispersion features a quadratic band touching and corresponding Berry
flux protected by particle-hole and discrete rotation symmetries. We also
construct an alternative particle-hole symmetric state---distinct in the
presence of inversion symmetry---without Berry flux. As in the Dirac composite
Fermi liquid introduced by Son, breaking particle-hole symmetry recovers the
familiar Chern-Simons theory. We discuss realizations of this phase both in 2D
and on bosonic topological insulator surfaces, as well as signatures in
experiments and simulations.Comment: 8 pages, 5 figure
Algebraic vortex liquid in spin-1/2 triangular antiferromagnets: Scenario for Cs_2CuCl_4
Motivated by inelastic neutron scattering data on Cs_2CuCl_4, we explore
spin-1/2 triangular lattice antiferromagnets with both spatial and easy-plane
exchange anisotropies, the latter due to an observed Dzyaloshinskii-Moriya
interaction. Exploiting a duality mapping followed by a fermionization of the
dual vortex degrees of freedom, we find a novel "critical" spin-liquid phase
described in terms of Dirac fermions with an emergent global SU(4) symmetry
minimally coupled to a non-compact U(1) gauge field. This ``algebraic vortex
liquid" supports gapless spin excitations and universal power-law correlations
in the dynamical spin structure factor which are consistent with those observed
in Cs_2CuCl_4. We suggest future neutron scattering experiments that should
help distinguish between the algebraic vortex liquid and other spin liquids and
quantum critical points previously proposed in the context of Cs_2CuCl_4.Comment: 4 pages, 3 figures; minor revisions, momenta in Fig. 2 correcte
Robust Helical Edge Transport in Quantum Spin Hall Quantum Wells
We show that burying of the Dirac point in semiconductor-based
quantum-spin-Hall systems can generate unexpected robustness of edge states to
magnetic fields. A detailed band-structure analysis reveals
that InAs/GaSb and HgTe/CdTe quantum wells exhibit such buried Dirac points. By
simulating transport in a disordered system described within an effective
model, we further demonstrate that buried Dirac points yield nearly quantized
edge conduction out to large magnetic fields, consistent with recent
experiments.Comment: 11 pages, 6 figure
Theory of the algebraic vortex liquid in an anisotropic spin-(1/2) triangular antiferromagnet
We explore spin-(1/2) triangular antiferromagnets with both easy-plane and lattice exchange anisotropies by employing a dual vortex mapping followed by a fermionization of the vortices. Over a broad range of exchange anisotropy, this approach leads naturally to a "critical" spin liquid—the algebraic vortex liquid—which appears to be distinct from other known spin liquids. We present a detailed characterization of this state, which is described in terms of noncompact QED3 with an emergent SU(4) symmetry. Descendant phases of the algebraic vortex liquid are also explored, which include the Kalmeyer-Laughlin spin liquid, a variety of magnetically ordered states such as the well-known coplanar spiral state, and supersolids. In the range of exchange anisotropy where the "square lattice" Néel ground state arises, we demonstrate that anomalous "roton" minima in the excitation spectrum recently reported in series expansions can be accounted for within our approach
Interlayer coherent composite Fermi liquid phase in quantum Hall bilayers
Composite fermions have played a seminal role in understanding the quantum
Hall effect, particularly the formation of a compressible `composite Fermi
liquid' (CFL) at filling factor nu = 1/2. Here we suggest that in multi-layer
systems interlayer Coulomb repulsion can similarly generate `metallic' behavior
of composite fermions between layers, even if the electrons remain insulating.
Specifically, we propose that a quantum Hall bilayer with nu = 1/2 per layer at
intermediate layer separation may host such an interlayer coherent CFL, driven
by exciton condensation of composite fermions. This phase has a number of
remarkable properties: the presence of `bonding' and `antibonding' composite
Fermi seas, compressible behavior with respect to symmetric currents, and
fractional quantum Hall behavior in the counterflow channel. Quantum
oscillations associated with the Fermi seas give rise to a new series of
incompressible states at fillings nu = p/[2(p \pm 1)] per layer (p an integer),
which is a bilayer analogue of the Jain sequence.Comment: 4 pages, 3 figure
Noise-induced backscattering in a quantum-spin-Hall edge
Time-reversal symmetry suppresses electron backscattering in a
quantum-spin-Hall edge, yielding quantized conductance at zero temperature.
Understanding the dominant corrections in finite-temperature experiments
remains an unsettled issue. We study a novel mechanism for conductance
suppression: backscattering caused by incoherent electromagnetic noise.
Specifically, we show that an electric potential fluctuating randomly in time
can backscatter electrons inelastically without constraints faced by
electron-electron interactions. We quantify noise-induced corrections to the dc
conductance in various regimes and propose an experiment to test this scenario.Comment: 5+3 pages, 1 figure; shortened version to appear in PRL, added
reference
Explicit derivation of duality between a free Dirac cone and quantum electrodynamics in (2+1) dimensions
We explicitly derive the duality between a free electronic Dirac cone and quantum electrodynamics in (2+1) dimensions (QED_3) with N=1 fermion flavors. The duality proceeds via an exact, non-local mapping from electrons to dual fermions with long-range interactions encoded by an emergent gauge field. This mapping allows us to construct parent Hamiltonians for exotic topological-insulator surface phases, derive the particle-hole-symmetric field theory of a half-filled Landau level, and nontrivially constrain QED_3 scaling dimensions. We similarly establish duality between bosonic topological insulator surfaces and N=2 QED_3
Algebraic vortex liquid theory of a quantum antiferromagnet on the kagome lattice
There is growing evidence from both experiment and numerical studies that low
half-odd integer quantum spins on a kagome lattice with predominant
antiferromagnetic near neighbor interactions do not order magnetically or break
lattice symmetries even at temperatures much lower than the exchange
interaction strength. Moreover, there appear to be a plethora of low energy
excitations, predominantly singlets but also spin carrying, which suggest that
the putative underlying quantum spin liquid is a gapless ``critical spin
liquid'' rather than a gapped spin liquid with topological order. Here, we
develop an effective field theory approach for the spin-1/2 Heisenberg model
with easy-plane anisotropy on the kagome lattice. By employing a vortex duality
transformation, followed by a fermionization and flux-smearing, we obtain
access to a gapless yet stable critical spin liquid phase, which is described
by (2+1)-dimensional quantum electrodynamics (QED) with an emergent
flavor symmetry. The specific heat, thermal conductivity, and
dynamical structure factor are extracted from the effective field theory, and
contrasted with other theoretical approaches to the kagome antiferromagnet.Comment: 14 pages, 8 figure
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