14,014 research outputs found
Updated dispersion-theoretical analysis of the nucleon electromagnetic form factors
In the light of the new data on the various neutron and proton
electromagnetic form factors taken in recent years, we update the
dispersion-theoretical analysis of the nucleon electromagnetic form factors
from the mid-nineties. The parametrization of the spectral functions includes
constraints from unitarity, perturbative QCD, and recent measurements of the
neutron charge radius. We obtain a good description of most modern form factor
data, with the exception of the Jefferson Lab data on G_E^p/G_M^p in the
four-momentum transfer range Q^2=3...6 GeV^2. For the magnetic radii of the
proton and the neutron we find r_M^p = 0.857 fm and r_M^n = 0.879 fm, which is
consistent with the recent determinations using continued fraction expansions.Comment: 5 pages, 3 ps figures, final version, exp. errors in Figs. 1 and 3
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Novel evaluation of the two-pion contribution to the nucleon isovector form factors
We calculate the two-pion continuum contribution to the nucleon isovector
spectral functions drawing upon the new high statistics measurements of the
pion form factor by the CMD-2, KLOE, and SND collaborations. The general
structure of the spectral functions remains unchanged, but the magnitude
increases by about 10%. Using the updated spectral functions, we calculate the
contribution of the two-pion continuum to the nucleon isovector form factors
and radii. We compare the isovector radii with simple rho-pole models and
illustrate their strong underestimation in such approaches. Moreover, we give a
convenient parametrization of the result for use in future form factor
analyses.Comment: 9 pages, 2 eps figures, revtex4, CMD-2 and SND data included,
conclusions unchanged, version to appear in Phys. Lett.
Dispersion analysis of the nucleon form factors including meson continua
Dispersion relations provide a powerful tool to analyse the electromagnetic
form factors of the nucleon for all momentum transfers. Constraints from
meson-nucleon scattering data, unitarity, and perturbative QCD can be included
in a straightforward way. In particular, we include the 2pi, rho-pi, and KKbar
continua as independent input in our analysis and provide an error band for our
results. Moreover, we discuss two different methods to include the asymptotic
constraints from perturbative QCD. We simultaneously analyze the world data for
all four form factors in both the space-like and time-like regions and
generally find good agreement with the data. We also extract the nucleon radii
and the omega-NN coupling constants. For the radii, we generally find good
agreement with other determinations with the exception of the electric charge
radius of the proton which comes out smaller. The omega-NN vector coupling
constant is determined relatively well by the fits, but for the tensor coupling
constant even the sign can not be determined.Comment: 24 pages, 9 figure
Electromagnetic Structure of the Z_c(3900)
The observation of the exotic quarkonium state Z_c(3900) by the BESIII and
Belle collaborations supports the concept of hadronic molecules. Charmonium
states interpreted as such molecules would be bound states of heavy particles
with small binding energies. This motivates their description using an
effective theory with contact interactions. In particular, we focus on the
electromagnetic structure of the charged state Z_c(3900). Using first
experimental results concerning spin and parity, we interpret it as an S-wave
molecule and calculate the form factors as well as charge and magnetic radii up
to next-to-leading order. We also present first numerical estimations of some
of these observables at leading order.Comment: 5 pages, 4 figures, final version to appear in Phys. Lett.
Universal Properties of the Four-Boson System in Two Dimensions
We consider the nonrelativistic four-boson system in two dimensions
interacting via a short-range attractive potential. For a weakly attractive
potential with one shallow two-body bound state with binding energy B_2, the
binding energies B_N of shallow N-body bound states are universal and thus do
not depend on the details of the interaction potential. We compute the
four-body binding energies in an effective quantum mechanics approach. There
are exactly two bound states: the ground state with B_4^(0)=197.3(1)B_2 and one
excited state with B_4^(1)=25.5(1)B_2. We compare our results to recent
predictions for N-body bound states with large N>>1.Comment: 7 pages, 1 ps figure, references and discussion added, final versio
The design of incentives for health care providers in developing countries : contracts, competition, and cost control
The authors examine the design and limitations of incentives for health care providers to serve in rural areas in developing countries. Governments face two problems: it is costly to compensate well-trained urban physicians enough to relocate to rural areas, and it is difficult to ensure quality care when monitoring performance is costly or impossible. The goal of providing universal primary health care has been hard to meet, in part because of the difficulty of staffing rural medical posts with conscientious caregivers. The problem is providing physicians with incentives at a reasonable cost. Governments are often unable to purchase medical services of adequate quality even from civil servants. Using simple microeconomic models of contracts and competition, the authors examine questions about: a) The design of rural service requirements and options for newly trained physicians. b) The impact of local competition on the desirable level of training for new doctors. c) The incentive power that can be reasonably expected from explicit contracts. One problem a government faces is choosing how much training to give physicians it wants to send to rural areas. Training is costly, and a physician relocated to the countryside is outside the government's direct control. Should rural doctors face a ceiling on the prices they charge patients?Can it be enforced? The authors discuss factors to consider in determining how to pay rural medical workers but conclude that we might have to set realistic bounds on our expectations about delivering certain kinds of services. If we can identify reasons why the best that can be expected is not a particularly good, it might lead us to explore entirely different policy systems. Maybe it is too hard to run certain decentralized systems. Maybe we should focus on less ambitious but more readily achievable goals, such as providing basic infrastructure.
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