  Andreev bound states (ABS) occur in Josephson junctions when the total phase
of the Andreev and normal reflections is a multiple of $2\pi$. In ballistic
junctions with an applied voltage bias, a quasi-particle undergoes multiple
Andreev reflections before entering the leads, resulting in peaks in the
current-voltage $I(V)$ curve. Here we present a general model for Josephson
junctions with spin-active interlayers i.e., magnetic or topological materials
with broken time-reversal symmetry. We investigate how ABS change the peak
positions and shape of $I(V)$, which becomes asymmetric for a single incident
angle. We show how the angle-resolved $I(V)$ curve becomes a spectroscopic tool
for the chirality and degeneracy of ABS.
