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The formation of a deeply-bound K⁻pp state by the ³He(in-flight K⁻, n) reaction is investigated theoretically in a distorted-wave impulse approximation using the Green's function method. The expected inclusive and semi-exclusive spectra at p_K⁻ = 1.0 GeV/c and θ_n = 0° are calculated for the forthcoming J-PARC E15 experiment. We discuss these spectra with some K⁻-“pp” optical potentials, taking into account the energy-dependence of the imaginary part of the potentials by a phase space suppression factor.

The formation of a deeply-bound K^-pp state by the ³He(in-flight K^-, n) reaction is investigated theoretically in a distorted-wave impulse approximation using the Green's function method. The expected inclusive and semi-exclusive spectra at p_K^- = 1.0 GeV/c and θ_n = 0° are calculated for the forthcoming J-PARC E15 experiment. We discuss these spectra with some K^--"pp" optical potentials, taking into account the energy-dependence of the imaginary part of the potentials by a phase space suppression factor.

The nuclear isotopic structure can be understood easily via the intermediate-energy charge exchange reactions of (p, n) and ${(}^3$He, $t)$ type. In the current contribution, we present some results for charge exchange reactions induced by ³He on targets lying in mass region $18\le A\le 208$ within the theoretical framework of plane wave impulse approximation (PWIA) and distorted wave impulse approximation (DWIA). Here, the recoil effects in PWIA have also been considered. Particularly, the angular distributions and the unit cross-sections have been calculated and compared with the available data. Further, the importance of inclusion of the exchange contribution in these reactions is also considered, which eventually enhance the matching with data.

Composite particle, ${(}^{3}He,t)$, charge exchange reactions on targets ${}^{12}C$, ${}^{13}C$, ${}^{18}O$, ${}^{26}Mg$, ${}^{58}Ni$ and ${}^{118,120}Sn$ at 140 MeV/u beam energy have been analyzed by employing distorted wave impulse approximation (DWIA). Specifically, unit cross-section and angular distribution have been calculated using normal optical model potential (NOMP) and single folding optical model potential (SFOMP) for both relativistic and non-relativistic cases. The sensitivity of present results on exchange terms has also been examined and it is pertinent to report here that the inclusion of these effects reduces the cross-section in magnitude up to 60%, which in turn brings it closer to the data except for ${}^{12}C$.

The formation of a deeply-bound K^-pp state by the ³He(in-flight K^-, n) reaction is investigated theoretically in a distorted-wave impulse approximation using the Green's function method. The expected inclusive and semi-exclusive spectra at p_K^- = 1.0 GeV/c and θ_n = 0∘ are calculated for the forthcoming J-PARC E15 experiment. We discuss these spectra with some K^--"pp" optical potentials, taking into account the energy-dependence of the imaginary part of the potentials by a phase space suppression factor.

In the present contribution, we report on calculation of the Λ-hypernuclear production induced by the stopped kaon K^-. We performed the calculation within the framework of the distorted wave impulse approximation and used chirally motivated transition amplitudes for the microscopic description of the elementary kaon-nucleon process. The sensitivity of the model to several effects was tested with a special attention paid to the impact caused by variations of the initial kaon and final state pion wave functions. The calculated production rates are reported for target nuclei from Lithium to Oxygen.

Theoretical hypernuclear photoproduction spectra are demonstrated by choosing typical medium-heavy nuclear targets such as ²⁸Si, ⁴⁰Ca, and ⁵²Cr. The predictions provide us with interesting opportunities of spectroscopic study beyond p-shell on the dynamical coupling between a hyperon and nuclear core excitations.

Theoretical hypernuclear photoproduction spectra are demonstrated by choosing typical medium-heavy nuclear targets such as ²⁸Si, ⁴⁰Ca, and ⁵²Cr. The predictions provide us with interesting opportunities of spectroscopic study beyond p-shell on the dynamical coupling between a hyperon and nuclear core excitations.