Neutral current photon emission reactions with nucleons and nuclei are studied. These processes are important backgrounds for νµ → νe (νµ →νe) appearance oscillation experiments where electromagnetic showers instigated by electrons (positrons) and photons are not distinguishable. At intermediate energies, these reactions are dominated by the weak excitation of the ∆(1232) resonance and its subsequent decay into N γ. There are also non-resonant contributions that, close to threshold, are fully determined by the effective chiral Lagrangian of strong interactions. In addition, we have also included mechanisms mediated by nucleon excitations (N * ) from the second resonance region above the ∆(1232). From these states, the contribution of the D13 N * (1520) turns out to be sizable for (anti)neutrino energies above 1.5 GeV. We have extended the model to nuclear targets taking, into account Pauli blocking, Fermi motion and the in-medium ∆ resonance broadening. We present our predictions for both the incoherent and coherent channels, showing the relevance of the nuclear corrections. We also discuss the target mass dependence of the cross sections. This study is important in order to reduce systematic effects in neutrino oscillation experiments.
In this paper, we present a review of recent works on weak decay of heavy mesons and baryons with two mesons, or a meson and a baryon, interacting strongly in the final state. The aim is to learn about the interaction of hadrons and how some particular resonances are produced in the reactions. It is shown that these reactions have peculiar features and act as filters for some quantum numbers which allow to identify easily some resonances and learn about their nature. The combination of basic elements of the weak interaction with the framework of the chiral unitary approach allow for an interpretation of results of many reactions and add a novel information to different aspects of the hadron interaction and the properties of dynamically generated resonances.
We have studied the J=ψϕ mass distribution of the B þ → J=ψϕK þ reaction from threshold to about 4250 MeV, and find that one needs the contribution of the Xð4140Þ with a narrow width, together with the Xð4160Þ which accounts for most of the strength of the distribution in that region. The existence of a clear cusp at the D Ã sD Ã s threshold indicates that the Xð4160Þ resonance is strongly tied to the D Ã sD Ã s channel, which finds a natural interpretation in the molecular picture of this resonance.
Based on previous studies that support the important role of the N * (2120)D13 resonance in the γp → K + Λ(1520) reaction, we make a re-analysis of this Λ(1520) photoproduction reaction taking into account the recent CLAS differential cross-section data. In addition to the contact, t−channel K exchange, s−channel nucleon pole and N * (2120) [previously called N * (2080)] resonance contributions, which have been already considered in previous works, we also study the u−channel Λ(1115) hyperon pole term. The latter mechanism has always been ignored in all theoretical analysis, which has mostly relied on the very forward K + angular LEPS data. It is shown that when the contributions from the N * (2120) resonance and the Λ(1115) hyperon are taken into account, both the new CLAS and the previous LEPS data can be simultaneously described. We also show that the contribution from the u−channel Λ(1115) pole term produces an enhancement for large K + angles, and it becomes more and more relevant as the photon energy increases, being essential to describe the CLAS differential cross sections at backward angles. Furthermore, we find that the new CLAS data also favor the existence of the N * (2120) resonance, and that these measurements can be used to further constrain its properties.PACS numbers: 13.75.Cs.; 14.20.-c.; 13.60.Rj.
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