For the potentials with a barrier the analytical continuation of the B
ohr - Sommerfeld quantization rule into the region of overbarrier reso
nances is derived. The equations obtained are valid for an arbitrary a
nalytical potential satisfying the quasiclassical conditions and deter
mine both the position of resonance E(r) and its width GAMMA. The resu
lts are demonstrated for a number of model potentials and also for the
Stark effect in a strong field. The energy asymptotic of resonances i
n the strong coupling regime is found.