1,264 research outputs found
Hadronic interactions from effective chiral Lagrangians of quarks and gluons
Effective chiral Lagrangians involving constituent quarks, Goldstone bosons
and long-distance gluons are believed to describe the strong interactions in an
intermediate energy region between the confinement scale and the chiral
symmetry breaking scale. Baryons and mesons in such a description are bound
states of constituent quarks. We discuss the combined use of the techniques of
effective chiral field theory and of the field theoretic method known as
Fock-Tani representation to derive effective hadron interactions. The Fock-Tani
method is based on a change of representation by means of a unitary
transformation such that the composite hadrons are redescribed by
elementary-particle field operators. Application of the unitary transformation
on the microscopic quark-quark interaction derived from a chiral effective
Lagrangian leads to chiral effective interactions describing all possible
processes involving hadrons and their constituents. The formalism is
illustrated by deriving the one-pion-exchange potential between two nucleons
using the quark-gluon effective chiral Lagrangian of Manohar and Georgi. We
also present the results of a study of the saturation properties of nuclear
matter using this formalism
Production of charmed baryons in collisions close to their thresholds
Cross sections for the charm-production reactions , , , and are presented, for energies near their respective thresholds. The
results are based on a calculation performed in the meson-exchange framework in
close analogy to earlier studies of the J\"ulich group on the
strangeness-production reactions , , by connecting the two sectors via SU(4) flavor
symmetry. The cross sections are found to be in the order of
at energies of MeV above the respective thresholds, for all considered
channels. Complementary to meson-exchange, where the charmed baryons are
produced by the exchange of and mesons, a charm-production potential
derived in a quark model is employed for assessing uncertainties. The cross
sections predicted within that picture turned out to be significantly smaller.Comment: 17 pages, 7 figure
Charm production in antiproton-proton annihilation
We study the production of charmed mesons (D) and baryons (Lambda_c) in
antiproton-proton (app) annihilation close to their respective production
thresholds. The elementary charm production process is described by either
baryon/meson exchange or by quark/gluon dynamics. Effects of the interactions
in the initial and final states are taken into account rigorously. The
calculations are performed in close analogy to our earlier study on app ->
antiLambda-Lambda and app -> antiK-K by connecting the processes via SU(4)
flavor symmetry. Our predictions for the antiLambda_c-Lambda_c production cross
section are in the order of 1 to 7 mb, i.e. a factor of around 10-70 smaller
than the corresponding cross sections for antiLambda-Lambda However, they are
100 to 1000 times larger than predictions of other model calculations in the
literature. On the other hand, the resulting cross sections for antiD-D
production are found to be in the order of 10^{-2} -- 10^{-1} microbarn and
they turned out to be comparable to those obtained in other studies.Comment: 5 pages, 2 figures, Contribution to the proceedings of the 21st
European Conference on Few-Body Problems in Physics, Salamanca, Spain, 30
August - 3 September 201
The (3770) resonance and its production in
The production of a meson-pair in antiproton-proton ()
annihilation close to the production threshold is investigated, with special
emphasis on the role played by the (3770) resonance. The study is
performed in a meson-baryon model where the elementary charm production process
is described by baryon exchange. Effects of the interactions in the initial and
final states are taken into account rigorously, where the latter involves also
those due to the (3770). The predictions for the production
cross section are in the range of 30 -- 250 nb, the contribution from the
(3770) resonance itself amounts to roughly 20 -- 80 nb.Comment: 6 pages, 6 figure
Production of charmed pseudoscalar mesons in antiproton-proton annihilation
We study the production of charmed mesons (D, D_s) in antiproton-proton
annihilation close to the reaction thresholds. The elementary charm production
process is described by baryon exchange and in the constituent quark model,
respectively. Effects of the interactions in the initial and final states are
taken into account rigorously. The calculations are performed in close analogy
to our earlier study on pbarp to KbarK by connecting the processes via SU(4)
flavor symmetry. Our predictions for the DDbar production cross section are in
the order of 10^{-2} -- 10^{-1} mu b. They turned out to be comparable to those
obtained in other studies. The cross section for a D_sD_s pair is found to be
of the same order of magnitude despite the fact that its production in pbarp
scattering requires a two-step process.Comment: 15 pages, 13 figures, some typos corrected, some comments adde
Scattering of charmed baryons on nucleons
Chiral effective field theory is utilized for extrapolating results on the
interaction, obtained in lattice QCD at unphysical (large) quark
masses, to the physical point. The pion-mass dependence of the components that
constitute the potential up to next-to-leading order
(pion-exchange diagrams and four-baryon contact terms) is fixed by information
from lattice QCD simulations. No recourse to SU(3) or SU(4) flavor symmetry is
made. It is found that the results of the HAL QCD Collaboration for quark
masses corresponding to -- MeV imply a moderately attractive
interaction at MeV with scattering lengths of
fm for the as well as the partial waves. For such
an interaction the existence of a charmed counterpart of the hypertriton is
unlikely but four- and/or five-baryons systems with a baryon could
be indeed bound.Comment: 7 pages, 2 figures; table added, several comments adde
The Gerasimov-Drell-Hearn sum rule and the single-pion photoproduction multipole E0+ close to threshold
The long-standing discrepancy between the Gerasimov-Drell-Hearn sum rule and
the analysis of pion photoproduction multipoles is greatly diminished by use of
s-wave multipoles that are in accord with the predictions of chiral
perturbation theory and describe the experimental data in the threshold region.
The remaining difference may be due to contributions of channels with more
pions and/or heavier mesons whose contributions to the sum rule remain to be
investigated by a direct measurement of the photoabsorption cross sections.Comment: 9 pages, latex, 1 figure, to appear in Phys. Rev.
Exact Casimir Interaction Between Semitransparent Spheres and Cylinders
A multiple scattering formulation is used to calculate the force, arising
from fluctuating scalar fields, between distinct bodies described by
-function potentials, so-called semitransparent bodies. (In the limit
of strong coupling, a semitransparent boundary becomes a Dirichlet one.) We
obtain expressions for the Casimir energies between disjoint parallel
semitransparent cylinders and between disjoint semitransparent spheres. In the
limit of weak coupling, we derive power series expansions for the energy, which
can be exactly summed, so that explicit, very simple, closed-form expressions
are obtained in both cases. The proximity force theorem holds when the objects
are almost touching, but is subject to large corrections as the bodies are
moved further apart.Comment: 5 pages, 4 eps figures; expanded discussion of previous work and
additional references added, minor typos correcte
Equation of state of quark-nuclear matter
Quark-nuclear matter (QNM) is a many-body system containing hadrons and
deconfined quarks. Starting from a microscopic quark-meson coupling (QMC)
Hamiltonian with a density dependent quark-quark interaction, an effective
quark-hadron Hamiltonian is constructed via a mapping procedure. The mapping is
implemented with a unitary operator such that composites are redescribed by
elementary-particle field operators that satisfy canonical commutation
relations in an extended Fock space. Application of the unitary operator to the
microscopic Hamiltonian leads to effective, hermitian operators that have a
clear physical interpretation. At sufficiently high densities, the effective
Hamiltonian contains interactions that lead to quark deconfinement. The
equation of state of QNM is obtained using standard many-body techniques with
the effective quark-hadron Hamiltonian. At low densities, the model is
equivalent to a QMC model with confined quarks. Beyond a critical density, when
quarks start to deconfine, the equation of state predicted for QNM is softer
than the QMC equation of state with confined quarks.Comment: 10 pages, ws-procs9x6.cls (included), 2 eps figures, to appear in the
Proceedings of the Joint CSSM/JHF Workshop, Adelaide, March 14-21, 200
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