Narrow Results

The radiative capture ${}^{14}$C(p, $\gamma$)${}^{15}$N is analyzed within the framework of potential model (PM) and R-matrix framework. The capture cross-section was analyzed for non-resonant and resonant transitions within the pathways that involve radiative capture via electric dipole ($E1$), and magnetic dipole ($M1$) transitions. The non-resonant transitions include $E1$ via s- and d-wave capture. The resonant transitions include electric dipole ($E1$), and magnetic dipole ($M1$) from the three dominant resonant states above the threshold of p+${}^{14}$C to the ground state of ${}^{15}$N. Based on the total cross-section, the rates associated with p+${}^{14}$C $\to$${}^{15}$N+$\gamma$ have been analyzed. In this paper, the resonant capture rates dominate compared to the existing data because, at resonant energies the amplitude of the cross-sections have a dominant effect on the radiative capture rates within the T₉ = 1.