  Background: Cluster states in $^{13}$N are extremely difficult to measure due
to the unavailability of $^{9}$B+$\alpha$ elastic scattering data. Purpose:
Using $\beta$-delayed charged-particle spectroscopy of $^{13}$O, clustered
states in $^{13}$N can be populated and measured in the 3$\alpha$+p decay
channel. Method: One-at-a-time implantation/decay of $^{13}$O was performed
with the Texas Active Target Time Projection Chamber (TexAT TPC). 149 $\beta
3\alpha p$ decay events were observed and the excitation function in $^{13}$N
reconstructed. Results: Four previously unknown $\alpha$-decaying excited
states were observed in $^{13}$N at an excitation energy of 11.3 MeV, 12.4 MeV,
13.1 MeV and 13.7 MeV decaying via the 3$\alpha$+p channel. Conclusion: These
states are seen to have a [$^{9}\mathrm{B}(\mathrm{g.s}) \bigotimes \alpha$/
$p+^{12}\mathrm{C}(0_{2}^{+})$], [$^{9}\mathrm{B}(\frac{1}{2}^{+}) \bigotimes
\alpha$], [$^{9}\mathrm{B}(\frac{5}{2}^{+}) \bigotimes \alpha$] and
[$^{9}\mathrm{B}(\frac{5}{2}^{+}) \bigotimes \alpha$] structure respectively. A
previously-seen state at 11.8 MeV was also determined to have a
[$p+^{12}\mathrm{C}(\mathrm{g.s.})$/ $p+^{12}\mathrm{C}(0_{2}^{+})$] 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
$\alpha$-clustered $^{12}$C. Evidence of the $\frac{1}{2}^{+}$ state in $^{9}$B
was also seen to be populated by decays from $^{13}$N$^{\star}$.
