  By solving the 5-body Faddeev-Yakubovsky equations in configuration space
with realistic nuclear Hamiltonians we have studied the resonant states of
$^5$H isotope. Two different methods, allowing to bypass the exponentially
diverging boundary conditions, have been employed providing consistent results.
The existence of $^5$H broad J$^{\pi}$=1/2$^+$,3/2$^+$,5/2$^+$ states as
S-matrix poles has been confirmed and compared with the, also calculated,
resonant states in $^4$H isotope. We have established that the positions of
these resonances only mildly depend on the nuclear interaction model.
