321 research outputs found

    Study of N(1520)N(1520) and N(1535)N(1535) structures via γ∗p→N∗\gamma^*p\to N^* transitions

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    The helicity amplitudes of the N(1520)N(1520) and N(1535)N(1535) resonances in the γ∗p→N∗\gamma^*p\to N^* electromagnetic transition are studied in the constituent quark model using the impulse approximation, with the proton and resonances assumed to be in three-quark configurations. The comparison of theoretical results and experimental data on the helicity amplitudes A1/2A_{1/2}, A3/2A_{3/2}, and S1/2S_{1/2} indicates that the N(1520)N(1520) and N(1535)N(1535) resonances are primarily composed of three-quark L=1L=1 states but may contain additional components. However, it is improbable that contributions from meson clouds will be dominant at low Q2Q^2.Comment: 6 pages, 3 figure

    Axial transition form factors of octet baryons in the perturbative chiral quark model

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    We study the axial transition form factors GAB→B′(Q2)G_A^{B\to B'}(Q^2) as well as the axial charges gAB→B′g_A^{B\to B'} of the octet baryons in the perturbative chiral quark model~(PCQM) with including both the ground and excited states in the intermediate quark propagators. The PCQM results on the GAB→B′(Q2)G_A^{B\to B'}(Q^2) and the gAB→B′g_A^{B\to B'} are found in good agreement with the existing experimental data and the lattice-QCD values. And the study figures out that the GAB→B′(Q2)G_A^{B\to B'}(Q^2) for all transitions behave in the dipole-like form, which is dominantly caused by the three-quark core. The meson cloud with the ground state quark propagator also plays an extremely important role but results in a flat contribution. The excited state quark propagator contributing to the GAB→B′(Q2)G_A^{B\to B'}(Q^2) could be regarded as the higher order correction and it is very limited

    Feasibility studies of time-like proton electromagnetic form factors at PANDA at FAIR

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    Simulation results for future measurements of electromagnetic proton form factors at \PANDA (FAIR) within the PandaRoot software framework are reported. The statistical precision with which the proton form factors can be determined is estimated. The signal channel pˉp→e+e−\bar p p \to e^+ e^- is studied on the basis of two different but consistent procedures. The suppression of the main background channel, i.e.\textit{i.e.} pˉp→π+π−\bar p p \to \pi^+ \pi^-, is studied. Furthermore, the background versus signal efficiency, statistical and systematical uncertainties on the extracted proton form factors are evaluated using two different procedures. The results are consistent with those of a previous simulation study using an older, simplified framework. However, a slightly better precision is achieved in the PandaRoot study in a large range of momentum transfer, assuming the nominal beam conditions and detector performance
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