10,156 research outputs found
Low stress and safe handling of outdoor cattle - effective measures to improve work environment and avoid dangerous situations
Grazing cattle are needed to preserve 450 000 hectares of semi-natural grasslands of high biodiversity in Sweden. Keeping cattle outdoors promotes their health and possibili¬ties to conduct natural behaviors. Working with cattle on pasture however, can increase accident rates (Health and Safety Authority, 2011). During the last two years, five fatali¬ties and several accidents have occurred during handling of cattle in Sweden. A method, based on knowledge of the animals’ natural behavior, referred to as low stress stock han¬dling (LSS-method), has been introduced to Sweden for cattle handling (Atkinson, 2011). A handler who consistently uses this method prevents the use of hits, sticks, harsh voice or negative forceful handling techniques. A consistent predictable approach from the han¬dler creates consistent and predictable animal behavior in return. Cattle become more trusting with their handlers and consequently more cooperative. This positive interaction between human being and animal can lead to both a safer work situation and a better animal welfare. On two of five studied farms so far, the LSS-method was actually inter¬vened during the observations, resulted in a successful reversal of conflict behaviour. On farm1, a highly stressed heifer took over three hours in attempt to load into a transport. It was successfully loaded within an hour after the intervention. On another farm, five escaped cows that the farmer had attempted to capture unsuccessfully for three conse¬cutive weeks were successfully captured through using the LSS-method
Vector meson-vector meson interaction in a hidden gauge unitary approach
The formalism developed recently to study vector meson--vector meson
interaction, and applied to the case of , is extended to study the
interaction of the nonet of vector mesons among themselves. The interaction
leads to poles of the scattering matrix corresponding to bound states or
resonances. We show that 11 states (either bound or resonant) get dynamically
generated in nine strangeness-isospin-spin channels. Five of them can be
identified with those reported in the PDG, i.e., the , ,
, , and . The masses of the latter three
tensor states have been used to fine-tune the free parameters of the unitary
approach, i.e., the subtraction constants in evaluating the vector meson
-vector meson loop functions in the dimensional regularization scheme. The
branching ratios of these five dynamically generated states are found to be
consistent with data. The existence of the other six states should be taken as
predictions to be tested by future experiments.Comment: typos corrected; more discussions; one of the appendix rearrange
The stability and the shape of the heaviest nuclei
In this paper, we report a systematic study of the heaviest nuclei within the
relativistic mean field (RMF) model. By comparing our results with those of the
Hartree-Fock-Bogoliubov method (HFB) and the finite range droplet model (FRDM),
the stability and the shape of the heaviest nuclei are discussed. The
theoretical predictions as well as the existing experimental data indicate that
the experimentally synthesized superheavy nuclei are in between the fission
stability line, the line connecting the nucleus with maximum binding energy per
nucleon in each isotopic chain, and the -stability line, the line
connecting the nucleus with maximum binding energy per nucleon in each isobaric
chain. It is shown that both the fission stability line and the
-stability line tend to be more proton rich in the superheavy region.
Meanwhile, all the three theoretical models predict most synthesized superheavy
nuclei to be deformed.Comment: 6 pages, 7 figures, to appear in Journal of Physics
Pairwise wave interactions in ideal polytropic gases
We consider the problem of resolving all pairwise interactions of shock
waves, contact waves, and rarefaction waves in 1-dimensional flow of an ideal
polytropic gas. Resolving an interaction means here to determine the types of
the three outgoing (backward, contact, and forward) waves in the Riemann
problem defined by the extreme left and right states of the two incoming waves,
together with possible vacuum formation. This problem has been considered by
several authors and turns out to be surprisingly involved. For each type of
interaction (head-on, involving a contact, or overtaking) the outcome depends
on the strengths of the incoming waves. In the case of overtaking waves the
type of the reflected wave also depends on the value of the adiabatic constant.
Our analysis provides a complete breakdown and gives the exact outcome of each
interaction.Comment: 39 page
Clues for the existence of two resonances
The axial vector meson was studied within the chiral unitary
approach, where it was shown that it has a two-pole structure. We reanalyze the
high-statistics WA3 experiment at 63 GeV, which
established the existence of both and , and we show that
it clearly favors our two-pole interpretation. We also reanalyze the
traditional K-matrix interpretation of the WA3 data and find that the good fit
of the data obtained there comes from large cancellations of terms of unclear
physical interpretation.Comment: published version in PRD; typos corrected; title changed to "Clues
for the existence of two resonances
Two-photon and one photon-one vector meson decay widths of the , , , , and
We calculate the radiative decay widths, two-photon () and one
photon-one vector meson (), of the dynamically generated resonances
from vector meson-vector meson interaction in a unitary approach based on the
hidden-gauge Lagrangians. In the present paper we consider the following
dynamically generated resonances: , , ,
, , two strangeness=0 and isospin=1 states, and two
strangeness=1 and isospin=1/2 states. For the and we
reproduce the previous results for the two-photon decay widths and further
calculate their one photon-one vector decay widths. For the and
the calculated two-photon decay widths are found to be consistent
with data. The , and decay widths of
the , , , are compared with the
results predicted by other approaches. The and
decay rates of the are also calculated and compared with the
results obtained in the framework of the covariant oscillator quark model. The
results for the two states with strangeness=0, isospin=1 and two states with
strangeness=1, isospin=1/2 are predictions that need to be tested by future
experiments.Comment: More discussions about the relation between qqbar states and
dynamically generated states; version published in PRD
Generalized Jacobi Elliptic One-Monopole - Type A
We present new classical generalized one-monopole solution of the SU(2)
Yang-Mills-Higgs theory with the Higgs field in the adjoint representation. We
show that this generalized solution with -winding number and
-winding number is an axially symmetric Jacobi elliptic
generalization of the 't Hooft-Polyakov one-monopole. We construct this axially
symmetric one-monopole solution by generalizing the large distance asymptotic
solution of the 't Hooft-Polyakov one-monopole to the Jacobi elliptic functions
and solving the second order equations of motion numerically when the Higgs
potential is vanishing and non vanishing. These solutions are regular non-BPS
finite energy solutions.Comment: 17 pages, 5 figure
Leptogenesis with Friedberg-Lee Symmetry
We consider the symmetric Friedberg-Lee (FL) symmetry for the
neutrino sector and show that a specific FL translation leads to the
tribimaximal mixing pattern of the Maki-Nakagawa-Sakata (MNS) matrix. We also
apply the symmetry to the type-I seesaw framework and address the baryon
asymmetry of the universe through the leptogenesis mechanism. We try to
establish a relation between the net baryon asymmetry and CP phases included in
the MNS matrix.Comment: Talk given at International Workshop on Dark Matter, Dark Energy and
Matter-Antimatter Asymmetry, Hsinchu, Taiwan, 20-21 Nov. 2009, to be
published in Modern Physics Letters A, reference adde
Role of the (1535) in the and reactions
We study the and
reactions with a unitary chiral approach. We find that the unitary chiral
approach, which generates the dynamically, can describe the data
reasonably well, particularly the ratio of the integrated cross sections. This
study provides further support for the unitary chiral description of the
. We also discuss some subtle differences between the coupling
constants determined from the unitary chiral approach and those determined from
phenomenological studies.Comment: version to appear in PRC; certain features of the approach clarifie
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