Search results for "Isospin"

showing 10 items of 264 documents

New interpretation for theDs2*(2573)and the prediction of novel exotic charmed mesons

2010

In this manuscript we study the vector-vector interaction within the hidden-gauge formalism in a coupled channel unitary approach. In the sector $C=1$, $S=1$, $J=2$ we get a pole in the $T$ matrix around 2572 MeV that we identify with the ${D}_{s2}^{*}(2573)$, coupling strongly to the ${D}^{*}{K}^{*}({D}_{s}^{*}\ensuremath{\phi}(\ensuremath{\omega}))$ channels. In addition we obtain resonances in other exotic sectors which have not been studied before such as $C=1$, $S=\ensuremath{-}1$, $C=2$, $S=0$ and $C=2$, $S=1$. These ``flavor-exotic'' states are interpreted as ${D}^{*}{\overline{K}}^{*}$, ${D}^{*}{D}^{*}$, and ${D}_{s}^{*}{D}^{*}$ molecular states but have not been observed yet. In to…

PhysicsNuclear and High Energy PhysicsParticle physicsMeson010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyStrangenessQuantum numberCoupling (probability)01 natural sciencesOmega3. Good healthIsospin0103 physical sciencesVector meson010306 general physicsSpin-½Physical Review D
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Vector meson-vector meson interaction in a hidden gauge unitary approach

2008

The formalism developed recently to study vector meson-vector meson interaction, and applied to the case of rho rho, 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 f(0)(1370), f(0)(1710), f(2)(1270), f(2)(')(1525), and K-2(*)(1430). The masses of the latter three tensor states have been used to fine-tune the free parameters of the unitary approach, i.e., the subtrac…

PhysicsNuclear and High Energy PhysicsParticle physicsMesonHadronFísicaFOS: Physical sciencesElementary particleStrangenessQuarkoniumHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)IsospinBound stateHigh Energy Physics::ExperimentVector meson
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B meson spectroscopy

2008

We study the $B$ meson spectroscopy allowing the mixture of conventional $P$ wave quark-antiquark states and four-quark components. A similar picture was used to describe the new $D_J$ and $D_{sJ}$ open charm mesons. The four-quark components shift the masses of some positive parity $B_{sJ}$ states below their corresponding isospin preserving two-meson threshold and therefore they are expected to be narrow. Electromagnetic decay widths are analyzed.

PhysicsNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeP waveNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaParity (physics)High Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Particle decayHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)IsospinB mesonInvariant massHigh Energy Physics::ExperimentSpectroscopyNuclear Experiment
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Prediction of a $Z_c(4000)$ $D^* \bar D^*$ state and relationship to the claimed $Z_c(4025)$

2014

After discussing the OZI suppression of one light meson exchange in the interaction of $D^* \bar D^*$ with isospin I=1, we study the contribution of two pion exchange to the interaction and the exchange of a heavy vector $J/\psi$. We find this latter mechanism weak but enough to barely bind the system in J=2 with a mass around 4000 MeV, while the effect of the two pion exchange is a net attraction but weaker than that from $J/\psi$ exchange. We discuss this state and try to relate it to the $Z_c(4025)$ state, above the $D^* \bar D^*$ threshold, claimed in an experiment at BES from and enhancement of the $D^* \bar D^*$ distribution close to threshold. Together with the results from a recent …

PhysicsNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::PhenomenologyNuclear TheoryFOS: Physical sciencesState (functional analysis)High Energy Physics - PhenomenologyDistribution (mathematics)PionHigh Energy Physics - Phenomenology (hep-ph)IsospinHigh Energy Physics::ExperimentNuclear ExperimentBar (unit)
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Study of reactions disclosing hidden charm pentaquarks with or without strangeness

2016

We present results for five reactions, Lambda(b) -> J/psi K(-)p, Lambda(b) -> J/psi eta Lambda, Lambda(b) -> J/psi pi(-)p, Lambda(b) -> J/psi K-0 Lambda and Xi(-)(b) -> J/psi K-Lambda, where combining information from the meson baryon interaction, using the chiral unitary approach, and predictions made for molecular states of hidden charm, with or without strangeness, we can evaluate invariant mass distributions for the light meson baryon states, and for those of J/psi p or J/psi Lambda. We show that with the present available information, in all of these reactions one finds peaks where the pentaquark states show up. In the Lambda(b) -> J/psi K(-)p, and Lambda(b) -> J/psi pi(-)p reactions w…

PhysicsNuclear and High Energy PhysicsParticle physicsMesonUnitarity010308 nuclear & particles physicsStrangenessLambda01 natural sciencesPseudoscalar mesonPentaquarkNuclear physicsBaryonIsospin0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsNuclear Physics A
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Weak pion production off the nucleon

2007

We develop a model for the weak pion production off the nucleon, which besides the Delta pole mechanism (weak excitation of the $\Delta(1232)$ resonance and its subsequent decay into $N\pi$), includes also some background terms required by chiral symmetry. We re-fit the $C_5^A(q^2)$ form factor to the flux averaged $\nu_\mu p \to \mu^-p\pi^+$ ANL $q^2-$differential cross section data, finding a substantially smaller contribution of the Delta pole mechanism than traditionally assumed in the literature. Within this scheme, we calculate several differential and integrated cross sections, including pion angular distributions, induced by neutrinos and antineutrinos and driven both by charged and…

PhysicsNuclear and High Energy PhysicsParticle physicsNeutral currentHadronFOS: Physical sciencesFísicaParity (physics)Nuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PionIsospinHigh Energy Physics::ExperimentNeutrinoNucleonCharged currentPhysical Review D
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Effects of Strong and Electromagnetic Correlations on Neutrino Interactions in Dense Matter

1998

An extensive study of the effects of correlations on both charged and neutral current weak interaction rates in dense matter is performed. Both strong and electromagnetic correlations are considered.The propagation of particle-hole interactions in the medium plays an important role in determining the neutrino mean free paths. The effects due to Pauli-Blocking and density, spin, and isospin correlations in the medium significantly reduce the neutrino cross sections. Due to the lack of experimental information at high density, these correlations are necessarily model dependent. For example, spin correlations in nonrelativistic models are found to lead to larger suppressions of neutrino cross …

PhysicsNuclear and High Energy PhysicsParticle physicsNeutral currentNuclear TheoryAstrophysics::High Energy Astrophysical PhenomenaAstrophysics (astro-ph)FOS: Physical sciencesWeak interactionNuclear matterAstrophysicsNuclear physicsNuclear Theory (nucl-th)Neutron starIsospinNeutrinoNucleonSpin-½
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Semiphenomenological approach to nucleon properties in nuclear-matter

1992

We have evaluated the nucleon self-energy in a model that has proper analytical properties, satisfies the low density theorem and provides values of Im \ensuremath{\Sigma} for high densities comparable to those of realistic microscopic approaches. The model, however, relies only upon the NN experimental cross sections and the empirical spin-isospin interaction, which induces an important polarization of the medium. The results obtained for the spectral functions, occupation numbers, and effective masses are quite reasonable. The model does not give the absolute value of the nucleon self-energy but only differences with respect to the Fermi energy. On the other hand, it provides an easy and …

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryFísicaElementary particleFermi energyFermionNuclear matterBaryonSelf-energyIsospinNucleon
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Tz = ±1 → 0 ISOSPIN SYMMETRY GAMOW-TELLER TRANSITIONS IN pf-SHELL NUCLEI

2010

Studying the Gamow-Teller (GT) transitions of stable as well as unstable pf-shell nuclei is one of the key issues in nuclear and astro-nuclear physics. Under the assumption that isospin T is a good quantum number, symmetry is expected for mirror nuclei and the GT transitions starting from the mirror nuclei. We study the GT transitions starting from Tz = ±1 mirror nuclei, respectively, by means of hadronic (3 He , t) charge-exchange reactions and complementary β decays.

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryHadronShell (structure)General Physics and AstronomyAstronomy and AstrophysicsKey issuesSymmetry (physics)Nuclear physicsGood quantum numberIsospinMirror nucleiNuclear ExperimentModern Physics Letters A
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Coherent two pion photoproduction on C-12

1997

We develop the formalism for coherent two pion photoproduction in nuclei and perform actual calculations of cross sections for $\pi^-\pi^+$ and $\pi^0\pi^0$ photoproduction on $^{12}C$. We find that due to the isospin symmetry the cross section for $\pi^0\pi^0$ production is very small and has a maximum when the pions propagate together. However, the kinematical region where the energies and polar angles of the two $\pi^0$ mesons are equal and their relative azimuthal angle $\phi=180^0$ is forbidden. Conversely in the $\pi^-\pi^+$ production the pions prefer to have a relative azimuthal angle 180$^0$ and the production of the pions propagating together is suppressed. The dominant one-body m…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryMesonNuclear TheoryFOS: Physical sciencesFísicaSymmetry (physics)Nuclear Theory (nucl-th)RenormalizationPionIsospinIsobarProduction (computer science)High Energy Physics::ExperimentNuclear ExperimentExcitation
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