Angular-Correlation Studies for theC12(He3, αγ)C11,C12(He3, pγ)N14, andO18(p, αγ)N15Reactions

Abstract
The particle-gamma angular correlation method of Litherland and Ferguson was used to gain information on the decay modes and spin assignments of the C11 2.00-MeV level; the N14 5.83- and 7.03-MeV levels; and the N15 5.28-, 6.33-, 8.31-, and 8.57-MeV levels. The C12(He3, α)C11, C12(He3, p)N14, and O18(p, α)N15 reactions were used to populate the levels. Protons and α particles were detected in an annular counter at 170° to the beam and gamma rays were detected at angles between 20 and 90° to the beam. The spin of the C11 2.00-MeV level was found to be ½, 32, or 52 with the quadrupole-dipole mixing parameter of the 2.00 → 0 transition given by x=+(0.27±0.07), or |x|>11 for 32 and x=(0.18±0.07) for 52. The angular distribution of the N14 7.03 → 0 transition gave 0.15<~x<~1.15 for this J=2 to J=1 transition. A 7.03 → 3.95 transition was observed with a branching ratio of 9±5%. The results for the N14 5.83-MeV level were consistent with earlier work. The N15 5.28-MeV level was assigned Jπ=52(+) with a value of - (0.15±0.06) or + (6.1±1.4) for the octupole-quadrupole mixing ratio of the 5.28 → 0 transition. The N15 6.33-MeV level was assigned Jπ=32() with a value of + (0.090.03+0.06) or + (1.40.4+0.1) for the 6.33 → 0 mixing ratio. Most probable assignments of ½+ and 32+ are made to the N15 8.31- and 8.57-MeV levels on the basis of this and previous work. The results are compared to shell-model predictions.