267 research outputs found
Exclusive production in proton-nucleus collisions
The exclusive meson production in a proton-nucleus collision, leading
to two body final states, is investigated in a fully covariant two-nucleon
model based on the effective Lagrangian picture. The explicit kaon production
vertex is described via creation, propagation and decay into relevant channel
of (1650), (1710) and (1720) intermediate baryonic states in the
initial collision of the projectile nucleon with one of its target counterparts
which is modeled by the one-pion exchange process. The calculated cross
sections show strong sensitivity to the medium effects on pion propagator and
to the final hypernuclear state excited in the reaction.Comment: Two new figures, version accepted for publication by Phys. Rev.
Ab initio approach to s-shell hypernuclei 3H_Lambda, 4H_Lambda, 4He_Lambda and 5He_Lambda with a Lambda N-Sigma N interaction
Variational calculations for s-shell hypernuclei are performed by explicitly
including degrees of freedom. Four sets of YN interactions (SC97d(S),
SC97e(S), SC97f(S) and SC89(S)) are used. The bound-state solution of
He is obtained and a large energy expectation value of the tensor
transition part is found. The internal energy of the
He subsystem is strongly affected by the presence of a particle
with the strong tensor transition potential.Comment: Phys. Rev. Lett. 89, 142504 (2002
Variational calculations of the -seperation energy of the O hypernucleus
Variational Monte Carlo calculations have been made for the O hypernucleus using realistic two- and three-baryon
interactions. A two pion exchange potential with spin- and space-exchange
components is used for the N potential. Three-body two-pion exchange
and strongly repulsive dispersive NN interactions are also included.
The trial wave function is constructed from pair- and triplet-correlation
operators acting on a single particle determinant. These operators consist of
central, spin, isospin, tensor and three- baryon potential components. A
cluster Monte Carlo method is developed for noncentral correlations and is used
with up to four-baryon clusters in our calculations. The three-baryon
NN force is discussed.Comment: 24 pages, 2 figs available by fax., for publication in Phys. Rev.
Phenomenological Lambda-Nuclear Interactions
Variational Monte Carlo calculations for (ground and
excited states) and are performed to decipher information on
-nuclear interactions. Appropriate operatorial nuclear and
-nuclear correlations have been incorporated to minimize the
expectation values of the energies. We use the Argonne two-body
NN along with the Urbana IX three-body NNN interactions. The study demonstrates
that a large part of the splitting energy in () is
due to the three-body NN forces. hypernucleus is
analyzed using the {\it s}-shell results. binding to nuclear matter
is calculated within the variational framework using the
Fermi-Hypernetted-Chain technique. There is a need to correctly incorporate the
three-body NN correlations for binding to nuclear matter.Comment: 18 pages (TeX), 2 figure
Possibility of \Lambda\Lambda pairing and its dependence on background density in relativistic Hartree-Bogoliubov model
We calculate a \Lambda\Lambda pairing gap in binary mixed matter of nucleons
and \Lambda hyperons within the relativistic Hartree-Bogoliubov model. Lambda
hyperons to be paired up are immersed in background nucleons in a normal state.
The gap is calculated with a one-boson-exchange interaction obtained from a
relativistic Lagrangian. It is found that at background density
\rho_{N}=2.5\rho_{0} the \Lambda\Lambda pairing gap is very small, and that
denser background makes it rapidly suppressed. This result suggests a
mechanism, specific to mixed matter dealt with relativistic models, of its
dependence on the nucleon density. An effect of weaker \Lambda\Lambda
attraction on the gap is also examined in connection with revised information
of the \Lambda\Lambda interaction.Comment: 8 pages, 6 figures, REVTeX 4; substantially rewritten, emphasis is
put on the LL pairing in pure neutron matte
A Realistic Description of Nucleon-Nucleon and Hyperon-Nucleon Interactions in the SU_6 Quark Model
We upgrade a SU_6 quark-model description for the nucleon-nucleon and
hyperon-nucleon interactions by improving the effective meson-exchange
potentials acting between quarks. For the scalar- and vector-meson exchanges,
the momentum-dependent higher-order term is incorporated to reduce the
attractive effect of the central interaction at higher energies. The
single-particle potentials of the nucleon and Lambda, predicted by the G-matrix
calculation, now have proper repulsive behavior in the momentum region q_1=5 -
20 fm^-1. A moderate contribution of the spin-orbit interaction from the
scalar-meson exchange is also included. As to the vector mesons, a dominant
contribution is the quadratic spin-orbit force generated from the rho-meson
exchange. The nucleon-nucleon phase shifts at the non-relativistic energies up
to T_lab=350 MeV are greatly improved especially for the 3E states. The
low-energy observables of the nucleon-nucleon and the hyperon-nucleon
interactions are also reexamined. The isospin symmetry breaking and the Coulomb
effect are properly incorporated in the particle basis. The essential feature
of the Lambda N - Sigma N coupling is qualitatively similar to that obtained
from the previous models. The nuclear saturation properties and the
single-particle potentials of the nucleon, Lambda and Sigma are reexamined
through the G-matrix calculation. The single-particle potential of the Sigma
hyperon is weakly repulsive in symmetric nuclear matter. The single-particle
spin-orbit strength for the Lambda particle is very small, in comparison with
that of the nucleons, due to the strong antisymmetric spin-orbit force
generated from the Fermi-Breit interaction.Comment: Revtex v2.09, 69 pages with 25 figure
Predicting the demand of physician workforce: an international model based on "crowd behaviors"
<p>Abstract</p> <p>Background</p> <p>Appropriateness of physician workforce greatly influences the quality of healthcare. When facing the crisis of physician shortages, the correction of manpower always takes an extended time period, and both the public and health personnel suffer. To calculate an appropriate number of Physician Density (PD) for a specific country, this study was designed to create a PD prediction model, based on health-related data from many countries.</p> <p>Methods</p> <p>Twelve factors that could possibly impact physicians' demand were chosen, and data of these factors from 130 countries (by reviewing 195) were extracted. Multiple stepwise-linear regression was used to derive the PD prediction model, and a split-sample cross-validation procedure was performed to evaluate the generalizability of the results.</p> <p>Results</p> <p>Using data from 130 countries, with the consideration of the correlation between variables, and preventing multi-collinearity, seven out of the 12 predictor variables were selected for entry into the stepwise regression procedure. The final model was: PD = (5.014 - 0.128 Ă proportion under age 15 years + 0.034 Ă life expectancy)<sup>2</sup>, with R<sup>2 </sup>of 80.4%. Using the prediction equation, 70 countries had PDs with "negative discrepancy", while 58 had PDs with "positive discrepancy".</p> <p>Conclusion</p> <p>This study provided a regression-based PD model to calculate a "norm" number of PD for a specific country. A large PD discrepancy in a country indicates the needs to examine physician's workloads and their well-being, the effectiveness/efficiency of medical care, the promotion of population health and the team resource management.</p
A relativistic two-nucleon model for reaction
We investigate the reaction within a covariant two
nucleon model. We focus on amplitudes which are described by creation,
propagation and decay into relevant channel of (1650), (1710), and
(1720) intermediate baryonic resonance states in the initial collision of
the projectile nucleon with one of its target counterparts. This collision is
modeled by the exchange of as well as and mesons. The
bound state nucleon and hyperon wave functions are obtained by solving the
Dirac equation with appropriate scalar and vector potentials. Expressions for
the reaction amplitudes are derived taking continuum particle wave functions in
both distorted wave and plane wave approximations. Detailed numerical results
are presented in the plane wave approximation; estimates of the effects of the
initial and final state interactions are given in the eikonal approximation.
Cross sections of 1 - 2 nb/sr at the peak positions, are obtained for favored
transitions in case of heavier targets.Comment: 36 pages including 14 figures, revised version, more discussions
added, to appear in Nucl. Phys.
First observation of the hyper superheavy hydrogen 6{\Lambda}H
Three candidate events of the neutron-rich hypernucleus 6{\Lambda}H were
uniquely identified in the FINUDA experiment at DA{\Phi}NE, Frascati, by
observing {\pi}+ mesons from the (K-stop,{\pi}+) production reaction on 6Li
targets, in coincidence with {\pi}-mesons from 6{\Lambda}H \rightarrow
6He+{\pi}- weak decay. Details of the experiment and the analysis of its data
are reported, leading to an estimate of (2.9\pm2.0)\cdot10-6/K- stop for the
6{\Lambda}H production rate times the two-body {\pi}- weak decay branching
ratio. The 6{\Lambda}H binding energy with respect to 5H + {\Lambda} was
determined jointly from production and decay to be B{\Lambda} = (4.0 \pm 1.1)
MeV, assuming that 5H is unbound with respect to 3H + 2n by 1.7 MeV. The
binding energy determined from production is higher, in each one of the three
events, than that determined from decay, with a difference of (0.98 \pm 0.74)
MeV here assigned to the 0+g.s. \rightarrow 1+ excitation. The consequences of
this assignment to {\Lambda} hypernuclear dynamics are briefly discussed.Comment: 20 pages, 8 figures, version matching published Nuclear Physics A
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