TY - JOUR
T1 - Cross Section Measurements of Two-nucleon Pickup Reactions in the 13C+d System at Deuteron Energies below 350 keV
AU - Naqvi, A. A.
AU - Nagadi, M. M.
AU - Kidwai, S.
AU - Al-Ohali, M. A.
AU - Khiari, F. Z.
PY - 1998
Y1 - 1998
N2 - Cross sections of two-nucleon pickup reactions in the 13C+d system, i.e. 13C(d, α0) 11B and 13C(d, α1)11B* reactions have been measured for 180-350 keV deuterons. The angular distributions were measured in steps of 20 keV at 14 angles ranging from 30° to 164°, while the excitation functions were measured at 90° in steps of 10 keV. The excitation functions of 13C(d, α0)11B and 13C(d, α1)11B* reactions with 5-167 and 3-307 MeV Q-values, respectively, exhibit smooth variations of cross section with energy. The angular distribution of 13C(d, α0)11B reaction is asymmetric. With decreasing deuteron energy, the degree of asymmetry increases and below 220 keV deuteron energy the angular distribution is backward-peaked. This indicates a dominating contribution from the direct reaction in this channel below 220 keV deuteron energy. The angular distribution of 13C(d, α1)11B* reactions are highly symmetric about 90°, indicating a dominating compound nucleus contribution over this energy range. The trends of angular distribution of 13C(d, α0)11B and 13C(d, α1)11B* are consistent with the results of Putt (1971) at higher deuteron energies.
AB - Cross sections of two-nucleon pickup reactions in the 13C+d system, i.e. 13C(d, α0) 11B and 13C(d, α1)11B* reactions have been measured for 180-350 keV deuterons. The angular distributions were measured in steps of 20 keV at 14 angles ranging from 30° to 164°, while the excitation functions were measured at 90° in steps of 10 keV. The excitation functions of 13C(d, α0)11B and 13C(d, α1)11B* reactions with 5-167 and 3-307 MeV Q-values, respectively, exhibit smooth variations of cross section with energy. The angular distribution of 13C(d, α0)11B reaction is asymmetric. With decreasing deuteron energy, the degree of asymmetry increases and below 220 keV deuteron energy the angular distribution is backward-peaked. This indicates a dominating contribution from the direct reaction in this channel below 220 keV deuteron energy. The angular distribution of 13C(d, α1)11B* reactions are highly symmetric about 90°, indicating a dominating compound nucleus contribution over this energy range. The trends of angular distribution of 13C(d, α0)11B and 13C(d, α1)11B* are consistent with the results of Putt (1971) at higher deuteron energies.
UR - http://www.scopus.com/inward/record.url?scp=0005578243&partnerID=8YFLogxK
U2 - 10.1071/p98035
DO - 10.1071/p98035
M3 - Article
AN - SCOPUS:0005578243
SN - 0004-9506
VL - 51
SP - 903
EP - 911
JO - Australian Journal of Physics
JF - Australian Journal of Physics
IS - 6
ER -