  Starting from the SU(3) limit, we consider the nature of the dynamically
generated resonances $\Lambda(1380)$, $\Lambda(1405)$ and $\Lambda(1680)$ as
the pion and kaon masses are tuned to their physical values. We show that the
accidental symmetry of the two octets due to the leading order
Weinberg-Tomozawa term is broken by the next-to-leading order terms. Most
interestingly, we observe an interchange of the two trajectories of the
$\Lambda(1380)$ and the $\Lambda(1405)$ away from the SU(3) limit at
next-to-leading order. This remarkable phenomenon can be investigated using
lattice QCD calculations that start from the SU(3) limit.
