The radiative capture [Formula: see text]C(p, [Formula: see text])[Formula: see text]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 ([Formula: see text]), and magnetic dipole ([Formula: see text]) transitions. The non-resonant transitions include [Formula: see text] via s- and d-wave capture. The resonant transitions include electric dipole ([Formula: see text]), and magnetic dipole ([Formula: see text]) from the three dominant resonant states above the threshold of p[Formula: see text]+[Formula: see text][Formula: see text]C to the ground state of [Formula: see text]N. Based on the total cross-section, the rates associated with p[Formula: see text][Formula: see text]+[Formula: see text][Formula: see text]C[Formula: see text] [Formula: see text][Formula: see text][Formula: see text]N[Formula: see text]+[Formula: see text][Formula: see text] 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.
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