3,185 research outputs found
Exploring psychosocial predictors of STI testing in University students
Peer reviewedPublisher PD
VLBA Continuum and H I Absorption Observations of the Ultra-Luminous Infrared Galaxy IRAS 17208-0014
We present phase-referenced VLBI observations of the radio continuum emission
from, and the neutral hydrogen 21 cm absorption toward, the Ultra-Luminous
Infrared Galaxy IRAS 17208-0014. The observations were carried out at 1362 MHz
using the Very Long Baseline Array, including the phased Very Large Array as an
element. The high-resolution radio continuum images reveal a nuclear starburst
region in this galaxy, which is composed of diffuse emission approximately 670
x 340 pc on the plane of the sky, and a number of compact sources. These
sources are most likely to be clustered supernova remnants and/or luminous
radio supernovae. Their brightness temperatures range over (2.2-6.6) x 10^{5}
K, with radio spectral luminosities between (1-10) x 10^{21} W Hz^{-1}. The
total VLBI flux density of the starburst region is ~52 mJy, which is about 50%
of the total flux density detected with the VLA at arcsecond resolution. For
this galaxy, we derive a massive star formation rate of ~84pm13 M{_\odot}
yr^{-1}, and a supernova rate of ~4pm1 yr^{-1}. H I absorption is detected in
multiple components with optical depths ranging between 0.3 and 2.5, and
velocity widths between 58 and 232 km s^{-1}. The derived column densities,
assuming T_{s}=100 K, range over (10-26) x 10^{21} cm^{-2}. The H I absorption
shows a strong velocity gradient of 453 km s^{-1} across 0.36 arcsec (274 pc).
Assuming Keplerian motion, the enclosed dynamical mass is about 2.3 x 10^9
sin^{-2}i M{_\odot}, comparable to the enclosed dynamical mass estimated from
CO observations.Comment: 26 pages total, 6 figures. ApJ accepted. To appear in the April 1,
2003 issue of ApJ. For a version with better images, see
http://www.aoc.nrao.edu/~emomjian/IRAS.p
Catalytic Dehydrogenation of Amine-Boranes using Geminal Phosphino-Boranes
The reaction of the intramolecular frustrated Lewis pair (FLP) tBu2PCH2BPh2 with the amine-boranes NH3·BH3 and Me2NH·BH3 leads to the formation of the corresponding FLP-H2 adducts as well as novel five-membered heterocycles that result from capturing the in situ formed amino-borane by a second equivalent of FLP. The sterically more demanding tBu2PCH2BMes2 does not form such a five-membered heterocycle when reacted with Me2NH·BH3 and its H2 adduct liberates dihydrogen at elevated temperatures, promoting the metal-free catalytic dehydrogenation of amine-boranes.Peer reviewe
Field induced stationary state for an accelerated tracer in a bath
Our interest goes to the behavior of a tracer particle, accelerated by a
constant and uniform external field, when the energy injected by the field is
redistributed through collision to a bath of unaccelerated particles. A non
equilibrium steady state is thereby reached. Solutions of a generalized
Boltzmann-Lorentz equation are analyzed analytically, in a versatile framework
that embeds the majority of tracer-bath interactions discussed in the
literature. These results --mostly derived for a one dimensional system-- are
successfully confronted to those of three independent numerical simulation
methods: a direct iterative solution, Gillespie algorithm, and the Direct
Simulation Monte Carlo technique. We work out the diffusion properties as well
as the velocity tails: large v, and either large -v, or v in the vicinity of
its lower cutoff whenever the velocity distribution is bounded from below.
Particular emphasis is put on the cold bath limit, with scatterers at rest,
which plays a special role in our model.Comment: 20 pages, 6 figures v3:minor corrections in sec.III and added
reference
Yukawa coupling unification and non-universal gaugino mediation of supersymmetry breaking
The requirement of Yukawa coupling unification highly constrains the SUSY
parameter space. In several SUSY breaking scenarios it is hard to reconcile
Yukawa coupling unification with experimental constraints from B(b->s gamma)
and the muon anomalous magnetic moment a_mu. We show that b-tau or even t-b-tau
Yukawa unification can be satisfied simultaneously with b->s gamma and a_mu in
the non-universal gaugino mediation scenario. Non-universal gaugino masses
naturally appear in higher dimensional grand unified models in which gauge
symmetry is broken by orbifold compactification. Relations between SUSY
contributions to fermion masses, b->s gamma and a_mu which are typical for
models with universal gaugino masses are relaxed. Consequently, these
phenomenological constraints can be satisfied simultaneously with a relatively
light SUSY spectrum, compared to models with universal gaugino masses.Comment: 20 pages, 8 figures. References added. A copy of the paper with
better resolution figures can be found at
http://www.hep.fsu.edu/~balazs/Physics/Papers/2003
Magnetic moments of light nuclei from Lattice Quantum Chromodynamics
We present the results of lattice QCD calculations of the magnetic moments of the lightest nuclei, the deuteron, the triton, and 3 He , along with those of the neutron and proton. These calculations, performed at quark masses corresponding to m π ∼ 800 MeV , reveal that the structure of these nuclei at unphysically heavy quark masses closely resembles that at the physical quark masses. In particular, we find that the magnetic moment of 3 He differs only slightly from that of a free neutron, as is the case in nature, indicating that the shell-model configuration of two spin-paired protons and a valence neutron captures its dominant structure. Similarly a shell-model-like moment is found for the triton, μ 3 H ∼ μ p . The deuteron magnetic moment is found to be equal to the nucleon isoscalar moment within the uncertainties of the calculations. Furthermore, deviations from the Schmidt limits are also found to be similar to those in nature for these nuclei. These findings suggest that at least some nuclei at these unphysical quark masses are describable by a phenomenological nuclear shell model
Family Unification on an Orbifold
We construct a family-unified model on a Z_2xZ_2 orbifold in five dimensions.
The model is based on a supersymmetric SU(7) gauge theory. The gauge group is
broken by orbifold boundary conditions to a product of grand unified SU(5) and
SU(2)xU(1) flavor symmetry. The structure of Yukawa matrices is generated by an
interplay between spontaneous breaking of flavor symmetry and geometric factors
arising due to field localization in the extra dimension.Comment: 13 page
The I=2 pipi S-wave Scattering Phase Shift from Lattice QCD
The pi+pi+ s-wave scattering phase-shift is determined below the inelastic
threshold using Lattice QCD. Calculations were performed at a pion mass of
m_pi~390 MeV with an anisotropic n_f=2+1 clover fermion discretization in four
lattice volumes, with spatial extent L~2.0, 2.5, 3.0 and 3.9 fm, and with a
lattice spacing of b_s~0.123 fm in the spatial direction and b_t b_s/3.5 in the
time direction. The phase-shift is determined from the energy-eigenvalues of
pi+pi+ systems with both zero and non-zero total momentum in the lattice volume
using Luscher's method. Our calculations are precise enough to allow for a
determination of the threshold scattering parameters, the scattering length a,
the effective range r, and the shape-parameter P, in this channel and to
examine the prediction of two-flavor chiral perturbation theory: m_pi^2 a r =
3+O(m_pi^2/Lambda_chi^2). Chiral perturbation theory is used, with the Lattice
QCD results as input, to predict the scattering phase-shift (and threshold
parameters) at the physical pion mass. Our results are consistent with
determinations from the Roy equations and with the existing experimental phase
shift data.Comment: 22 pages, 16 figure
Incidental finding of a giant intracardiac angioma infiltrating both ventricles in a 35-year-old woman: a case report
Background: Primary cardiac tumors are rare and often asymptomatic or present with unspecific symptoms. Benign cardiac tumors of vascular origin are especially rare, with only few existing data in the literature. Case presentation: A 35-year-old Caucasian female patient presented to our department with an asymptomatic giant intracardiac angioma infiltrating both ventricles. Evaluation of this tumor involved electrocardiography, echocardiography, cardiac magnetic resonance imaging, coronary angiography, an open myocardial biopsy, and histological examination of the resected specimen. Because our patient was asymptomatic, she was managed conservatively with regular follow-up. We discuss the treatment options available in comparison with similar cases. Conclusion: Diagnosis and therapy of benign cardiac tumors, especially of asymptomatic lesions, can be a challenge. There is no evidence available to help in the management of such patients. An extensive evaluation is needed with different imaging modalities, and case-specific decisions should be made that involve experts in cardiology, cardio-oncology, and heart surgery
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