  The existence of near-threshold charmed baryon $\Lambda_c(2595)^+$ implies
that the pion and the lightest, isospin-$1$ charmed baryon $\Sigma_c$ interact
very strongly at extremely low energies. Using the two-flavor version of heavy
hadron chiral perturbation theory, I explore the direct consequences of this
strong force by investigating whether the $\Sigma_c$ can trap two very soft
pions to form any visible hadronic states. The answer is positive. It is found
without tuning any free parameters or ultraviolet cutoff that the state in
question, with quantum numbers $I(J^P) = 1({\frac{1}{2}}^+)$, presents itself
as a resonance pole only a few MeVs away from the $\pi \pi \Sigma_c$ threshold.
Subleading corrections are estimated with power-counting arguments, and the
smallness of pion momenta is found to facilitate the reliability of the
analysis. Because of its proximity in mass, this excited $\Sigma_c$ resonance
is speculated to be related to the broad resonance labeled as
$\Lambda_c^+(2765)$.
