1,861 research outputs found
Non-localities and Fermi motion corrections in atoms
We evaluate the p-wave amplitudes from the chiral Lagrangians and from
there construct the p-wave part of the nucleus optical potential plus a
small s-wave part induced from the elementary p-wave amplitude and the nuclear
Fermi motion. Simultaneously, the momentum and energy dependence of the s-wave
optical potential, previously developed, are taken into account and shown to
generate a small p-wave correction to the optical potential. All the
corrections considered are small compared to the leading s-wave potential, and
lead to changes in the shifts and widths which are smaller than the
experimental errors.
A thorough study of the threshold region and low densities is conducted,
revealing mathematical problems for which a physical solution is given.Comment: revised version, 28 pages, Latex, 8 postscript figures. Submitted to
Nucl. Phys.
Quark-mass dependence of baryon resonances
We study the quark-mass dependence of J^P = \frac12^- s-wave and J^P =
\frac32^- d-wave baryon resonances. Parameter-free results are obtained in
terms of the leading order chiral Lagrangian. In the 'heavy' SU(3) limit with
m_\pi =m_K \simeq 500 MeV the s-wave resonances turn into bound states forming
two octets plus a singlet representations of the SU(3) group. Similarly the
d-wave resonances turn into bound states forming an octet and a decuplet in
this limit. A contrasted result is obtained in the 'light' SU(3) limit with
m_\pi =m_K \simeq 140 MeV for which no resonances exist.Comment: 8 pages, three figures, talk presented at HYP200
Chiral Symmetry and s-wave Low-Lying Meson-Baryon Resonances
The wave meson-baryon scattering is analyzed for the isospin-strangeness
and sectors, in a Bethe-Salpeter coupled channel
formalism incorporating Chiral Symmetry. For both sectors, four channels have
been considered: , , , and ,
, , , respectively. The needed two particle
irreducible matrix amplitudes are taken from lowest order Chiral Perturbation
Theory in a relativistic formalism. There appear undetermined low energy
constants, as a consequence of the renormalization of the amplitudes, which are
obtained from fits to the available data: elastic phase-shifts, and cross sections and to
mass-spectrum, the elastic and
--matrices and to the
cross section data. The position and residues of the complex poles in the
second Riemann sheet of the scattering amplitude determine masses, widths and
branching ratios of the (1535) and (1650) and
(1405) and (1670) resonances, in reasonable agreement with
experiment. A good overall description of data, from threshold up to around 2
GeV is achieved despite the fact that three-body channels have not been
explicitly included.Comment: 5 Pages, 2 figures, invited contribution to Focus Session on Nature
of Threshold N*, to be published in Proceedings of Nstar 2002, Pittsburgh,
USA, October 9-12, 2002 (World Scientific
Odd Parity Light Baryon Resonances
We use a consistent SU(6) extension of the meson-baryon chiral Lagrangian
within a coupled channel unitary approach in order to calculate the T-matrix
for meson-baryon scattering in s-wave. The building blocks of the scheme are
the pion and nucleon octets, the rho nonet and the Delta decuplet. We identify
poles in this unitary T-matrix and interpret them as resonances. We study here
the non exotic sectors with strangeness S=0,-1,-2,-3 and spin J=1/2, 3/2 and
5/2. Many of the poles generated can be associated with known N, Delta, Sigma,
Lambda and Xi resonances with negative parity. We show that most of the
low-lying three and four star odd parity baryon resonances with spin 1/2 and
3/2 can be related to multiplets of the spin-flavor symmetry group SU(6). This
study allows us to predict the spin-parity of the Xi(1620), Xi(1690), Xi(1950),
Xi(2250), Omega(2250) and Omega(2380) resonances, which have not been
determined experimentally yet.Comment: New appendix and references adde
CHIRAL SYMMETRY CONSTRAINTS ON THE INTERACTION WITH THE NUCLEAR PION CLOUD
The real part of the selfenergy for the interaction of the
with the pion nuclear cloud is evaluated in lowest order of chiral perturbation
theory and is found to be exactly zero in symmetric nuclear matter. This
removes uncertainties in that quantity found in former phenomenological
analyses and is supported by present experimental data on nucleus
scattering.Comment: 11 pp, LaTeX file, 4 figures (appended as compressed tar files, uses
epsf.sty
Charmed hadrons in nuclear medium
We study the properties of charmed hadrons in dense matter within a
coupled-channel approach which accounts for Pauli blocking effects and meson
self-energies in a self-consistent manner. We analyze the behaviour in this
dense environment of dynamically-generated baryonic resonances as well as the
open-charm meson spectral functions. We discuss the implications of the
in-medium properties of open-charm mesons on the and the
predicted X(3700) scalar resonances.Comment: 4 pages, 5 figures, invited parallel talk in the 5th International
Conference on Quarks and Nuclear Physics (QNP09), Beijing, September 21-26,
200
Strange and charm mesons at FAIR
We study the properties of strange and charm mesons in hot and dense matter
within a self-consistent coupled-channel approach for the experimental
conditions of density and temperature expected for the CBM experiment at
FAIR/GSI. The in-medium solution at finite temperature accounts for Pauli
blocking effects, mean-field binding of all the baryons involved, and meson
self-energies. We analyze the behaviour in this hot and dense environment of
dynamically-generated baryonic resonances together with the evolution with
density and temperature of the strange and open-charm meson spectral functions.
We test the spectral functions for strange mesons using energy-weighted sum
rules and finally discuss the implications of the properties of charm mesons on
the D_{s0}(2317) and the predicted X(3700) scalar resonances.Comment: 12 pages, 9 figures, invited talk at XXXI Mazurian Lakes Conference
on Physics: Nuclear Physics and the Road to FAIR, August 30-September 6,
2009, Piaski, Polan
-Nucleus Scattering at Low and Intermediate Energies
We calculate -nucleus elastic differential, reaction and total cross
sections for different nuclei (C,Ca and Pb) at several
laboratory antikaon momenta, ranging from 127 MeV to 800 MeV. We use different
antikaon-nucleus optical potentials, some of them fitted to kaonic atom data,
and study the sensitivity of the cross sections to the considered
antikaon-nucleus dynamics.Comment: Only 4 pages, Latex, 3 Figures. This version is much shorter than the
previous one. Some details and references have been omitte
Chiral restoration from pionic atoms?
We evaluate widths and shifts of pionic atoms using a theoretical
microscopical potential in which the pion decay constant is changed by
an in--medium density dependent one (), predicted by different
partial Chiral restoration calculations. We show that the results obtained for
shifts and widths are worse than if this modification were not implemented. On
the other hand, we argue that in microscopic many body approaches for the pion
selfenergy, based on effective Lagrangians, the mechanisms responsible for the
change of in the medium should be automatically incorporated.
Therefore, the replacement of by in the many body
derivation of the microscopic potential would be inappropriate.Comment: 10 pages, new comments and references adde
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