21,836 research outputs found
The Top Triangle Moose
We introduce a deconstructed model that incorporates both Higgsless and
top-color mechanisms. The model alleviates the typical tension in Higgsless
models between obtaining the correct top quark mass and keeping delta-rho
small. It does so by singling out the top quark mass generation as arising from
a Yukawa coupling to an effective top-Higgs which develops a small vacuum
expectation value, while electroweak symmetry breaking results largely from a
Higgsless mechanism. As a result, the heavy partners of the SM fermions can be
light enough to be seen at the LHC.Comment: To appear in proceedings of SCGT09, Nagoya, Japan. 5 page
Lattice vibrations and structural instability in Cesium near the cubic to tetragonal transition
Under pressure cesium undergoes a transition from a high-pressure fcc phase
(Cs-II) to a collapsed fcc phase (Cs-III) near 4.2GPa. At 4.4GPa there follows
a transition to the tetragonal Cs-IV phase. In order to investigate the lattice
vibrations in the fcc phase and seek a possible dynamical instability of the
lattice, the phonon spectra of fcc-Cs at volumes near the III-IV transition are
calculated using Savrasov's density functional linear-response LMTO method.
Compared with quasiharmonic model calculations including non-central
interatomic forces up to second neighbours, at the volume (
is the experimental volume of bcc-Cs with =6.048{\AA}), the
linear-response calculations show soft intermediate wavelength
phonons. Similar softening is also observed for
short wavelength and phonons and intermediate
wavelength phonons. The Born-von K\'{a}rm\'{a}n analysis of
dispersion curves indicates that the interplanar force constants exhibit
oscillating behaviours against plane spacing and the large softening of
intermediate wavelength phonons results from a
negative (110)-interplanar force-constant . The frequencies of the
phonons with around 1/3 become imaginary
and the fcc structure becomes dynamically unstable for volumes below .
It is suggested that superstructures corresponding to the
soft mode should be present as a precursor of tetragonal Cs-IV structure.Comment: 12 pages, 5 figure
Coupled Magnetic Excitations in Single Crystal PrBa2Cu3O6.2
The dispersion of the low-energy magnetic excitations of the Pr sublattice in
PrBa2Cu3O6.2 is determined by inelastic neutron scattering measurements on a
single crystal. The dispersion, which shows the effect of interactions with the
Cu spin-waves, is well described by a model of the coupled Cu-Pr magnetic
system. This enables values for the principal exchange constants to be
determined, which suggest that both Pr-Pr and Cu-Pr interactions are important
in producing the anomalously high ordering temperature of the Pr sublattice.
Measurements of the Cu optic spin wave mode show that the inter-layer Cu-Cu
exchange is significantly lower than in YBa2Cu3O6.2.Comment: To be published Phys. Rev. Let
Plasmonic eigenmodes in individual and bow-tie graphene nanotriangles
Serving as a new two-dimensional plasmonic material, graphene has stimulated
an intensive study of its optical properties which benefit from the unique
electronic band structure of the underlying honeycomb lattice of carbon atoms.
In classical electrodynamics, nanostructured graphene is commonly modeled by
the computationally demanding problem of a three-dimensional conducting film of
atomic-scale thickness. Here, we propose an efficient alternative
two-dimensional electrostatic approach where all the calculation procedures are
restricted to the plane of the graphene sheet. To explore possible quantum
effects, we perform tight-binding calculations, adopting a random-phase
approximation. We investigate the multiple plasmon modes in triangles of
graphene, treating the optical response classically as well as quantum
mechanically in the case of both armchair and zigzag edge termination of the
underlying atomic lattice. Compared to the classical plasmonic spectrum which
is "blind" to the edge termination, we find that the quantum plasmon
frequencies exhibit blueshifts in the case of armchair edge termination, while
redshifts are found for zigzag edges. Furthermore, we find spectral features in
the zigzag case which are associated with electronic edge states not present
for armchair termination. Merging pairs of such triangles into dimers, the
plasmon hybridization leads to energy splitting in accordance with
plasmon-hybridization theory, with a lower energy for the antisymmetric modes
and a smaller splitting for modes with less confinement to the gap region. The
hybridization appears strongest in classical calculations while the splitting
is lower for armchair edges and even more reduced for zigzag edges. Our various
results illustrate a surprising phenomenon: Even 20 nm large graphene
structures clearly exhibit quantum plasmonic features due to atomic-scale
details in the edge termination.Comment: 27 pages including 7 figures. Supplementary information available
upon request to author
Stress Tensor from the Trace Anomaly in Reissner-Nordstrom Spacetimes
The effective action associated with the trace anomaly provides a general
algorithm for approximating the expectation value of the stress tensor of
conformal matter fields in arbitrary curved spacetimes. In static, spherically
symmetric spacetimes, the algorithm involves solving a fourth order linear
differential equation in the radial coordinate r for the two scalar auxiliary
fields appearing in the anomaly action, and its corresponding stress tensor. By
appropriate choice of the homogeneous solutions of the auxiliary field
equations, we show that it is possible to obtain finite stress tensors on all
Reissner-Nordstrom event horizons, including the extreme Q=M case. We compare
these finite results to previous analytic approximation methods, which yield
invariably an infinite stress-energy on charged black hole horizons, as well as
with detailed numerical calculations that indicate the contrary. The
approximation scheme based on the auxiliary field effective action reproduces
all physically allowed behaviors of the quantum stress tensor, in a variety of
quantum states, for fields of any spin, in the vicinity of the entire family (0
le Q le M) of RN horizons.Comment: 43 pages, 12 figure
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