  We study the in-gap states of the quantum dot hybridized to a conducting and
superconducting electrode. The usual proximity effect suppresses electronic
states over the entire subgap regime $|\omega| < \Delta$, where $\Delta$
denotes the energy gap of superconductor. Owing to the Andreev scattering there
can, however, emerge additional in-gap states whose line-broadening (inverse
life-time) depends on the coupling to a normal electrode. We show that even
number of such bound states appears in the quantum dot spectrum, depending on a
competition between the Coulomb repulsion and the induced on-dot pairing. We
discuss signatures of these in-gap states showing up in the tunneling
conductance, especially in a low-bias regime dominated by the Andreev channel.
