608 research outputs found
Modification of the Lifshitz-Kosevich formula for anomalous quantum oscillations in inverted insulators
It is generally believed that quantum oscillations are a hallmark of a Fermi
surface and the oscillations constitute the ringing of it. Recently, it was
understood that in order to have well defined quantum oscillations you do not
only not need well defined quasiparticles, but also the presence of a Fermi
surface is unnecessary. In this paper we investigate such a situation for an
inverted insulator from a analytical point of view. Even in the insulating
phase clear signatures of quantum oscillations are observable and we give a
fully analytical formula for the strongly modified Lifshitz-Kosevich amplitude
which applies in the clean as well as the disordered case at finite
temperatures.Comment: 8 figure
The antiferromagnetic Ising model on the swedenborgite lattice
Geometrical frustration in spin systems often results in a large number of
degenerate ground states. In this work we study the antiferromagnetic Ising
model on the three dimensional swedenborgite lattice which is a specific
stacking of Kagom\'e and triangular layers. The model contains two exchange
couplings, one within the Kagom\'e layer, another one in between Kagom\'e and
triangular layers. We determine the phase diagram with and without easy axis
magnetic field and calculate the ground state degeneracy explicitly in terms of
the residual entropy. At zero field we find two different ground state
manifolds separated by a first order transition at T = 0 and equal exchange
couplings. We also determine the T = 0 phase diagram in a magnetic field and
find a rich phase diagram with both degenerate and non-degenerate phases
depending on the field strength and out-of-plane coupling.Comment: 7 pages, 8 figure
Kondo effect in three-dimensional Dirac and Weyl systems
Magnetic impurities in three-dimensional Dirac and Weyl systems are shown to
exhibit a fascinatingly diverse range of Kondo physics, with distinctive
experimental spectroscopic signatures. When the Fermi level is precisely at the
Dirac point, Dirac semimetals are in fact unlikely candidates for a Kondo
effect due to the pseudogapped density of states. However, the influence of a
nearby quantum critical point leads to the unconventional evolution of Kondo
physics for even tiny deviations in the chemical potential. Separating the
degenerate Dirac nodes produces a Weyl phase: time-reversal symmetry-breaking
precludes Kondo due to an effective impurity magnetic field, but different
Kondo variants are accessible in time-reversal invariant Weyl systems.Comment: 4+ pages, 2 figure
Interplay of disorder and interactions in subcritically tilted and anisotropic three-dimensional Weyl fermions
We study the effects of disorder and Coulomb interactions on the physics of
three-dimensional type-I Weyl fermions with tilted and anisotropic dispersions
in a renormalization group approach. To lowest non-trivial loop order we show
that the tendency of the Coulomb interactions to restore the symmetry of the
dispersion in the semimetallic region of the phase diagram dominates the
stabilization of the tilt and anisotropy favored by weak disorder. We argue
that the topology of the renormalization flow of the disorder and Coulomb
couplings is essentially determined by gauge invariance, so that these findings
continue to hold qualitatively at any order in perturbation theory.Comment: 9+5 page
Gate-controlled Kondo screening in graphene: Quantum criticality and electron-hole asymmetry
Magnetic impurities in neutral graphene provide a realization of the
pseudogap Kondo model, which displays a quantum phase transition between phases
with screened and unscreened impurity moment. Here, we present a detailed study
of the pseudogap Kondo model with finite chemical potential mu. While carrier
doping restores conventional Kondo screening at lowest energies, properties of
the quantum critical fixed point turn out to influence the behavior over a
large parameter range. Most importantly, the Kondo temperature T_K shows an
extreme asymmetry between electron and hole doping. At criticality, depending
on the sign of mu, T_K follows either the scaling prediction T_K ~ |mu| with a
universal prefactor, or T_K ~ |mu|^x with x = 2.6. This asymmetry between
electron and hole doping extends well outside the quantum critical regime and
also implies a qualitative difference in the shape of the tunneling spectra for
both signs of mu.Comment: 6 pages, 6 figs; (v2) extended discussion of RG flow, final version
as publishe
Interaction effects on almost flat surface bands in topological insulators
We consider ferromagnetic instabilities of two-dimensional helical Dirac
fermions hosted on the surface of three-dimensional topological insulators. We
investigate ways to increase the role of interactions by means of modifying the
bulk properties which in turn changes both the surface Dirac theory and the
screening of interactions. We discuss both the long-ranged part of the Coulomb
interactions controlled by the dimensionless coupling constant as well as the effects of local
interactions parametrized by the ratio of
a local interaction on the surface, , and the surface
bandwidth, . If large compared to 1, both mechanisms can
induce spontaneously surface ferromagnetism, thereby gapping the surface Dirac
metal and inducing an anomalous quantum Hall effect. We investigate two
mechanisms which can naturally lead to small Fermi velocities
and a corresponding small bandwidth
at the surface when the bulk band gap is reduced. The same mechanisms can,
however, also lead to an enhanced screening of surface interactions. While in
all considered cases the long-ranged part of the Coulomb interaction is
screened efficiently, , we discuss situations, where
becomes \emph{parametrically}\ large
compared to 1, thus inducing surface magnetism.Comment: 15 pages, 8 figures, published version with minor updat
- …