Author/Authors :
A.T. Rudchik، نويسنده , , Yu.O. Shyrma، نويسنده , , K.W. Kemper، نويسنده , , K. Rusek، نويسنده , , E.I Koshchy، نويسنده , , S. Kliczewski، نويسنده , , B.G. Novatsky، نويسنده , , O.A. Ponkratenko، نويسنده , , E. Piasecki، نويسنده , , G.P. Romanyshyna، نويسنده , , Yu.M. Stepanenko، نويسنده , , I. Strojek، نويسنده , , S.B. Sakuta، نويسنده , , A. Budzanowski، نويسنده , , L. G?owacka، نويسنده , , I. Skwirczynska، نويسنده , , R. Siudak، نويسنده , , J. Choi?ski، نويسنده ,
Abstract :
Complete angular distributions of the 13C + 18O elastic and inelastic scattering were measured at the energy image (image). These and the 13C + 18O scattering data taken from the literature at the energies image were analyzed within the optical model and coupled-reaction-channels methods. Sets of Woods–Saxon 13C + 18O optical potential parameters were obtained. The 13C + 18O scattering data and deduced potential parameters are compared with those for 12C + 18O and 13C + 16O previously measured and analyzed. The 13C + 18O elastic scattering is well described by potential scattering over its complete angular range. The 13C + 18O inelastic-scattering data were well described over the entire angular range as arising from collective excitations of the states in the target and projectile nuclei.
Keywords :
NUCLEAR REACTIONS , 13C(18O , Measured elastic and inelastic ?(?)?(?) , Scattering mechanism features , Deduced potential parameters , 18O) , Optical model and coupled-reaction-channels analysis , View the MathML sourceElab(O18)=105 MeV
