7,279 research outputs found
Ballistic charge transport in chiral-symmetric few-layer graphene
A transfer matrix approach to study ballistic charge transport in few-layer
graphene with chiral-symmetric stacking configurations is developed. We
demonstrate that the chiral symmetry justifies a non-Abelian gauge
transformation at the spectral degeneracy point (zero energy). This
transformation proves the equivalence of zero-energy transport properties of
the multilayer to those of the system of uncoupled monolayers. Similar
transformation can be applied in order to gauge away an arbitrary magnetic
field, weak strain, and hopping disorder in the bulk of the sample. Finally, we
calculate the full-counting statistics at arbitrary energy for different
stacking configurations. The predicted gate-voltage dependence of conductance
and noise can be measured in clean multilayer samples with generic metallic
leads.Comment: 6 pages, 5 figures; EPL published versio
Elastic forward scattering in the cuprate superconducting state
We investigate the effect of elastic forward scattering on the ARPES spectrum
of the cuprate superconductors. In the normal state, small angle scattering
from out-of-plane impurities is thought to broaden the ARPES spectral response
with minimal effect on the resistivity or the superconducting transition
temperature . Here we explore how such forward scattering affects the
ARPES spectrum in the d-wave superconducting state. Away from the nodal
direction, the one-electron impurity scattering rate is found to be suppressed
as approaches the gap edge by a cancellation between normal and
anomalous scattering processes, leading to a square-root-like feature in the
spectral weight as approaches -\Delta_\k from below. For momenta
away from the Fermi surface, our analysis suggests that a dirty optimally or
overdoped system will still display a sharp but nondispersive peak which could
be confused with a quasiparticle spectral feature. Only in cleaner samples
should the true dispersing quasiparticle peak become visible. At the nodal
point on the Fermi surface, the contribution of the anomalous scattering
vanishes and the spectral weight exhibits a Lorentzian quasiparticle peak in
both energy and momentum.
Our analysis, including a treatment of unitary scatterers and inelastic spin
fluctuation scattering, suggests explanations for the sometimes mysterious
lineshapes and temperature dependences of the peak structures observed in the
\BSCCO system.Comment: 12 pages, 14 figure
Towards the electron EDM search: Theoretical study of HfF+
We report first ab initio relativistic correlation calculations of potential
curves for ten low-lying electronic states, effective electric field on the
electron and hyperfine constants for the ^3\Delta_1 state of cation of a heavy
transition metal fluoride, HfF^+, that is suggested to be used as the working
state in experiments to search for the electric dipole moment of the electron.
It is shown that HfF^+ has deeply bound ^1\Sigma^+ ground state, its
dissociation energy is D_e=6.4 eV. The ^3\Delta_1 state is obtained to be the
relatively long-lived first excited state lying about 0.2 eV higher. The
calculated effective electric field E_eff=W_d|\Omega| acting on an electron in
this state is 5.84*10^{24}Hz/(e*cm)Comment: 4 page
Andreev levels in a single-channel conductor
We calculate the subgap density of states of a disordered single-channel
normal metal connected to a superconductor at one end (NS junction) or at both
ends (SNS junction). The probability distribution of the energy of a bound
state (Andreev level) is broadened by disorder. In the SNS case the two-fold
degeneracy of the Andreev levels is removed by disorder leading to a splitting
in addition to the broadening. The distribution of the splitting is given
precisely by Wigner's surmise from random-matrix theory. For strong disorder
the mean density of states is largely unaffected by the proximity to the
superconductor, because of localization, except in a narrow energy region near
the Fermi level, where the density of states is suppressed with a log-normal
tail.Comment: 12 pages, 5 figure
Di-electrons from meson Dalitz decay in proton-proton collisions
The reaction is discussed within a
covariant effective meson-nucleon theory. The model is adjusted to data of the
subreaction . Our focus is on di-electrons from Dalitz decays
of mesons, , and the role of
the corresponding transition form factor . Numerical
results are presented for the intermediate energy kinematics of HADES
experiments
Spatial distribution of local currents of massless Dirac fermions in quantum transport through graphene nanoribbons
We employ the formalism of bond currents, expressed in terms of the
nonequilibrium Green functions, to image the charge flow between two sites of
the honeycomb lattice of graphene ribbons of few nanometers width. In sharp
contrast to nonrelativistic electrons, current density profiles of quantum
transport at energies close to the Dirac point in clean zigzag graphene
nanoribbons (ZGNR) differs markedly from the profiles of charge density peaked
at the edges due to zero-energy localized edge states. For transport through
the lowest propagating mode induced by these edge states, edge vacancies do not
affect current density peaked in the center of ZGNR. The long-range potential
of a single impurity acts to reduce local current around it while concurrently
increasing the current density along the zigzag edge, so that ZGNR conductance
remains perfect .Comment: 5 pages, 5 figure
Calculation of coupling constant g_phi-pi-gamma in QCD sum rules
The coupling constant of g_phi-pi-gamma decay is calculated in the method of
QCD sum rules. A comparison of our prediction on the coupling constant with the
result obtained from analysis of the experimental data is performed.Comment: 6 pages, 3 figure
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