# First observation of the $\beta$3$\alpha$p decay of $^{13}\mathrm{O}$ via $\beta$-delayed charged-particle spectroscopy

## TL;DR

This study reports the first direct observation of the rare $eta$-delayed 3$oldsymbol{ extalpha}$+p decay of $^{13} ext{O}$, revealing new $oldsymbol{ extalpha}$-decaying states and providing insights into exotic nuclear clustering phenomena.

## Contribution

It provides the first experimental evidence of $eta$-delayed 3$oldsymbol{ extalpha}$+p decay in $^{13} ext{O}$ and identifies four previously unknown $oldsymbol{ extalpha}$-decaying states.

## Key findings

- Observed 149 $eta$-delayed 3$oldsymbol{ extalpha}$+p events.
- Discovered four new $oldsymbol{ extalpha}$-decaying states in $^{13} ext{N}$.
- Confirmed the population of the $rac{1}{2}^{+}$ state in $^{9} ext{B}$.

## Abstract

Background: The $\beta$-delayed proton-decay of $^{13}\mathrm{O}$ has previously been studied, but the direct observation of $\beta$-delayed $\alpha$+$\alpha$+$\alpha$+p decay has not been reported. Purpose: Observing rare 3$\alpha$+p events from the decay of excited states in $^{13}\mathrm{N}^{\star}$ allows for a sensitive probe of exotic highly-clustered configurations in $^{13}$N. Method: To measure the low-energy products following $\beta$-delayed 3$\alpha$p-decay, the TexAT Time Projection Chamber was employed using the one-at-a-time $\beta$-delayed charged-particle spectroscopy technique at the Cyclotron Institute, Texas A&M University. Results: A total of $1.9 \times 10^{5}$ $^{13}\mathrm{O}$ implantations were made inside the TexAT Time Projection Chamber. 149 3$\alpha$+p events were observed yielding a $\beta$-delayed 3$\alpha+p$ branching ratio of 0.078(6)%. Conclusion: Four previously unknown $\alpha$-decaying states were observed, one with a strong $^{9}\mathrm{B(g.s)}+\alpha$ characteristic at 11.3 MeV, one with a $^{9}\mathrm{B}(\frac{1}{2}^{+})+\alpha$ nature at 12.4 MeV, and another two that are dominated by $^{9}\mathrm{B}({\frac{5}{2}}^{+})+\alpha$ at 13.1 and 13.7 MeV. Population of the $\frac{1}{2}^{+}$ state in $^{9}\mathrm{B}$ has been unambiguously seen, cementing the predicted existence of the mirror-state based on the states observed in $^{9}\mathrm{Be}$.