Properties of the 4.77- and 5.16-MeV States ofB10

Abstract
The energy levels in B10 at 4.77 and 5.16 MeV have been studied by means of the reactions B11(He3,α)B10 and Li6(α,γ)B10. In measurements on the B11(He3,α)B10 reaction (EHe3=3.5 MeV), alpha particles populating states of B10 were observed at 90° in coincidence with (a) B10 recoil nuclei, (b) B10 recoils and gamma rays, and (c) decay alpha particles, by using two solid-state detectors and a NaI detector. Relative alpha-particle and gamma-ray branching intensities were determined for the decay of the 4.77- and 5.16-MeV states. The ratio of population intensities of the 5.16- and 5.11-MeV states was measured by using a Buechner-type magnetic spectrograph. In the Li6(α,γ)B10 reaction thick-target gamma-ray yields were measured at resonances for forming the 4.77- and 5.16-MeV states. For the 4.77-MeV state the angular distribution of the predominant 4.05-MeV gamma ray was determined, the 4.77-MeV ground-state transition was detected, and the angular distribution of the 4.77-MeV gamma ray was measured. The intensity of the ground-state gamma-ray branch from the 4.77-MeV level was measured to be (0.5±0.1)%, and the angular distribution of this transition in the Li6(α,γ)B10 reaction favors an assignment of Jπ=3+ to the 4.77-MeV state. Assignments of either Jπ=2+ or 3+ are allowed by the angular distribution of the 4.05-MeV transition from this state. ΓγΓ for the 4.77-MeV level was measured to be (2.3±0.3)×103. For the Jπ=3+ assignment, partial widths for the 4.77-MeV level were measured to be Γγ=0.033±0.006 eV and Γα=14±3 eV. The partial widths of the 5.16-MeV level were measured as Γγ=2.9±1.1 eV and