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For the first time, the total yield and inclusive spectra of the $Delta^{++}(1232)$isobar are measured in $ u p$ and $ u n$ charged-current interactions. An indication is obtained that the $Delta^{++}(1232)$ production mainly results from the neutrino scattering on the valence d- quark of the target nucleon. The total yield of $Delta^{++}(1232)$ in $ u p$ interactions is compatible with that measured in hadronic interactions of the same net charge and net baryonic number. The yield of $Delta^{++}(1232)$ in $ u n$ interactions is significantly suppressed as compared to the case of the proton target. The form of the squared transverse momentum distributions, both in $ u p$ and $ u n$ interactions, is found to be compatible with the available data on the neutrinoproduction of $Lambda$ hyperon. The experimental data are compared with the LEPTO6.5 model predictions.
The reaction gamma p -> p pi0 gamma has been measured with the Crystal Ball / TAPS detectors using the energy-tagged photon beam at the electron accelerator facility MAMI-B. Energy and angular differential cross sections for the emitted photon gamma
Differential and total cross sections for the quasifree reactions $gamma prightarroweta p$ and $gamma nrightarroweta n$ have been determined at the MAMI-C electron accelerator using a liquid deuterium target. Photons were produced via bremsstrahlung
This paper focuses on a measurement of deeply virtual Compton scattering (DVCS) performed at Jefferson Lab using a nearly-6-GeV polarized electron beam, two longitudinally polarized (via DNP) solid targets of protons (NH3) and deuterons (ND3) and the
The atomic nucleus is made of protons and neutrons (nucleons), that are themselves composed of quarks and gluons. Understanding how the quark-gluon structure of a nucleon bound in an atomic nucleus is modified by the surrounding nucleons is an outsta
Experimental above-barrier fusion cross-sections for $^{17}$F + $^{12}$C are compared to the fusion excitation functions for $^{16,18}$O, $^{19}$F, and $^{20}$Ne ions on a carbon target. In comparing the different systems both the differing static si