Cluster structure of 3𝛼+𝑝 states in 13 N
Cluster states in 13 N are extremely difficult to measure due to the unavailability of 9 B +𝛼 elastic-scattering data. Using 𝛽-delayed charged-particle spectroscopy of 13 O, clustered states in 13 N can be populated and measured in the 3𝛼+𝑝 decay channel. One-at-a-time implantation and decay of 13 O was performed with the Texas Active Target Time Projection Chamber. 149𝛽3𝛼𝑝 decay events were observed and the excitation function in 13 N reconstructed. Four previously unknown 𝛼-decaying excited states were observed in 13 N at an excitation energy of 11.3, 12.4, 13.1, and 13.7 MeV decaying via the 3𝛼+𝑝 channel. These states are seen to have a [ 9 B (g.s) ⨂𝛼/𝑝 + 12 C (0$^+_2$)], [ 9 B ($\frac{1}{2}$ + ) ⨂𝛼], [ 9 B ($\frac{5}{2}$ + ) ⨂𝛼], and [ 9 B ($\frac{5}{2}$) ⨂𝛼] structure, respectively. A previously seen state at 11.8 MeV was also determined to have a [𝑝+ 12 C (g.s.)/𝑝+ 12 C (0$^+_2$)] structure. The overall magnitude of the clustering is not able to be extracted, however, due to the lack of a total width measurement. Clustered states in 13 N (with unknown magnitude) seem to persist from the addition of a proton to the highly 𝛼-clustered 12 C . Evidence of the $\frac{1}{2}$ + state in 9 B was also seen to be populated by decays from 13 N ★ .