  Phase- and voltage bias-sensitive quasiparticle transport at a double
$NIS_1IS_2$ interface is considered. The barriers $I$ range from tunnel to
transparent, and the intermediate region $S_1$ has a width comparable to the
superconducting coherence length. A phase difference $\varphi$ is applied to
the Josephson junction $S_1IS_2$. The normal and Andreev reflections at the
$NIS_1$ interface become $\varphi$-sensitive, and transport is governed by
interferences within the narrow $S_1$ region, both in the normal and anomalous
channels. The subgap conductance is separately (energy $E$)- and (phase
$\varphi$)- symmetric. Above the superconducting gap, the conductance is in
general not symmetric even if $(E,\varphi)$ is changed in $(-E,-\varphi)$, but
the symmetry is restored by averaging Fermi oscillations. The Tomasch
oscillations are amplified by the phase difference. The subgap conductance
exhibits a resonant structure at the energy of the Andreev bound states (ABS)
of the $S_1IS_2$ junction, providing a side-spectroscopy of such states.
Depending on the relative transparencies of the junctions, the resonance can
increase or reduce the conductance, and it can even vanish for $\varphi=\pi$,
featuring total reflection of quasiparticles at $NS_1$ by the ABS at $S_1S_2$.
