773 research outputs found
Magnetic effects in sulfur-decorated graphene
The interaction between two different materials can present novel phenomena
that are quite different from the physical properties observed when each
material stands alone. Strong electronic correlations, such as magnetism and
superconductivity, can be produced as the result of enhanced Coulomb
interactions between electrons. Two-dimensional materials are powerful
candidates to search for the novel phenomena because of the easiness of
arranging them and modifying their properties accordingly. In this work, we
report magnetic effects of graphene, a prototypical non-magnetic
two-dimensional semi-metal, in the proximity with sulfur, a diamagnetic
insulator. In contrast to the well-defined metallic behaviour of clean
graphene, an energy gap develops at the Fermi energy for the graphene/sulfur
compound with decreasing temperature. This is accompanied by a steep increase
of the resistance, a sign change of the slope in the magneto-resistance between
high and low fields, and magnetic hysteresis. A possible origin of the observed
electronic and magnetic responses is discussed in terms of the onset of
low-temperature magnetic ordering. These results provide intriguing insights on
the search for novel quantum phases in graphene-based compounds.Comment: 6 pages and 5 figure
Luther-Emery Stripes, RVB Spin Liquid Background and High Tc Superconductivity
The stripe phase in high Tc cuprates is modeled as a single stripe coupled to
the RVB spin liquid background by the single particle hopping process. In
normal state, the strong pairing correlation inherent in RVB state is thus
transfered into the Luttinger stripe and drives it toward spin-gap formation
described by Luther-Emery Model. The establishment of global phase coherence in
superconducting state contributes to a more relevant coupling to
Luther-Emery Stripe and leads to gap opening in both spin and charge sectors.
Physical consequences of the present picture are discussed, and emphasis is put
on the unification of different energy scales relevant to cuprates, and good
agreement is found with the available experimental results, especially in
ARPES.Comment: 4 pages, RevTe
Strained graphene: tight-binding and density functional calculations
We determine the band structure of graphene under strain using density
functional calculations. The ab-initio band strucure is then used to extract
the best fit to the tight-binding hopping parameters used in a recent
microscopic model of strained graphene. It is found that the hopping parameters
may increase or decrease upon increasing strain, depending on the orientation
of the applied stress. The fitted values are compared with an available
parametrization for the dependence of the orbital overlap on the distance
separating the two carbon atoms. It is also found that strain does not induce a
gap in graphene, at least for deformations up to 10%
Bosonization of interacting fermions in arbitrary dimension beyond the Gaussian approximation
We use our recently developed functional bosonization approach to bosonize
interacting fermions in arbitrary dimension beyond the Gaussian
approximation. Even in the finite curvature of the energy dispersion at
the Fermi surface gives rise to interactions between the bosons. In higher
dimensions scattering processes describing momentum transfer between different
patches on the Fermi surface (around-the-corner processes) are an additional
source for corrections to the Gaussian approximation. We derive an explicit
expression for the leading correction to the bosonized Hamiltonian and the
irreducible self-energy of the bosonic propagator that takes the finite
curvature as well as around-the-corner processes into account. In the special
case that around-the-corner scattering is negligible, we show that the
self-energy correction to the Gaussian propagator is negligible if the
dimensionless quantities are
small compared with unity for all patches . Here is the cutoff
of the interaction in wave-vector space, is the Fermi wave-vector,
is the chemical potential, is the usual dimensionless Landau
interaction-parameter, and is the {\it{local}} density of
states associated with patch . We also show that the well known
cancellation between vertex- and self-energy corrections in one-dimensional
systems, which is responsible for the fact that the random-phase approximation
for the density-density correlation function is exact in , exists also in
, provided (1) the interaction cutoff is small compared with
, and (2) the energy dispersion is locally linearized at the Fermi the
Fermi surface. Finally, we suggest a new systematic method to calculate
corrections to the RPA, which is based on the perturbative calculation of the
irreducible bosonic self-energy arising from the non-Gaussian terms of the
bosonized Hamiltonian.Comment: The abstract has been rewritten. No major changes in the text
Theory of Fermion Liquids
We develop a general theory of fermion liquids in spatial dimensions greater
than one. The principal method, bosonization, is applied to the cases of short
and long range longitudinal interactions, and to transverse gauge interactions.
All the correlation functions of the system may be obtained with the use of a
generating functional. Short-range and Coulomb interactions do not destroy the
Landau Fermi fixed point. Novel fixed points are found, however, in the cases
of a super-long range longitudinal interaction in two dimensions and transverse
gauge interactions in two and three spatial dimensions. We consider in some
detail the 2+1-dimensional problem of a Chern-Simons gauge action combined with
a longitudinal two-body interaction which
controls the density, and hence gauge, fluctuations. For we find that
the gauge interaction is irrelevant and the Landau fixed point is stable, while
for the interaction is relevant and the fixed point cannot be accessed
by bosonization. Of special importance is the case (Coulomb
interaction) which describes the Halperin-Lee-Read theory of the half-filled
Landau level. We obtain the full quasiparticle propagator which is of a
marginal Fermi liquid form. Using Ward Identities, we show that neither the
inclusion of nonlinear terms in the fermion dispersion, nor vertex corrections,
alters our results: the fixed point is accessible by bosonization. As the
two-point fermion Green's function is not gauge invariant, we also investigate
the gauge-invariant density response function. Near momentum , in
addition to the Kohn anomaly we find singular behavior. In Appendices we
present a numerical calculation of the spectral function for a Fermi liquid
with Landau parameter . We also show how Kohn's theorem isComment: Minor corrections and clarifications, and additional references. 30
pages, RevTex 3.0, 3 figures in uuencoded postscript files
Cyclotron motion in graphene
We investigate cyclotron motion in graphene monolayers considering both the
full quantum dynamics and its semiclassical limit reached at high carrier
energies. Effects of zitterbewegung due to the two dispersion branches of the
spectrum dominate the irregular quantum motion at low energies and are obtained
as a systematic correction to the semiclassical case. Recent experiments are
shown to operate in the semiclassical regime.Comment: 6 pages, 1 figure include
Conductivity of graphene: How to distinguish between samples with short and long range scatterers
Applying a quasiclassical equation to carriers in graphene we found a way how
to distinguish between samples with the domination of short and long range
scatterers from the conductivity measurements. The model proposed explains
recent transport experiments with chemically doped as well as suspended
graphene.Comment: 6 pages, 3 figures, some references have been corrected and revise
Effect of Coulomb interactions on the physical observables of graphene
We give an update of the situation concerning the effect of electron-electron
interactions on the physics of a neutral graphene system at low energies. We
revise old renormalization group results and the use of 1/N expansion to
address questions of the possible opening of a low-energy gap, and the
magnitude of the graphene fine structure constant. We emphasize the role of
Fermi velocity as the only free parameter determining the transport and
electronic properties of the graphene system and revise its renormalization by
Coulomb interactions in the light of recent experimental evidence.Comment: Proceedings of the Nobel Symposium on graphene 2010, to appear as a
special issue in Physica Script
Terahertz imaging and spectroscopy of large-area single-layer graphene
We demonstrate terahertz (THz) imaging and spectroscopy of a 15x15-mm^2
single-layer graphene film on Si using broadband THz pulses. The THz images
clearly map out the THz carrier dynamics of the graphene-on-Si sample, allowing
us to measure sheet conductivity with sub-mm resolution without fabricating
electrodes. The THz carrier dynamics are dominated by intraband transitions and
the THz-induced electron motion is characterized by a flat spectral response. A
theoretical analysis based on the Fresnel coefficients for a metallic thin film
shows that the local sheet conductivity varies across the sample from {\sigma}s
= 1.7x10^-3 to 2.4x10^-3 {\Omega}^-1 (sheet resistance, {\rho}s = 420 - 590
{\Omega}/sq).Comment: 6 pages, 5 figure
The Physics of Kondo Impurities in Graphene
This article summarizes our understanding of the Kondo effect in graphene,
primarily from a theoretical perspective. We shall describe different ways to
create magnetic moments in graphene, either by adatom deposition or via
defects. For dilute moments, the theoretical description is in terms of
effective Anderson or Kondo impurity models coupled to graphene's Dirac
electrons. We shall discuss in detail the physics of these models, including
their quantum phase transitions and the effect of carrier doping, and confront
this with existing experimental data. Finally, we point out connections to
other quantum impurity problems, e.g., in unconventional superconductors,
topological insulators, and quantum spin liquids.Comment: 27 pages, 8 figs. Review article prepared for Rep. Prog. Phys. ("key
issues" section). (v2) Final version as publishe
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