  Poor man's Majoranas (PMMs) hold the promise to engineer Majorana bound
states in a highly tunable setup consisting of a chain of quantum dots that are
connected via superconductors. Due to recent progress in controlling the
amplitudes of elastic cotunneling (ECT) and crossed Andreev reflection (CAR),
two vital ingredients for PMMs, experimental investigations of PMMs have gained
significant interest. Previously, analytic conditions for the "sweet spots"
that result in PMMs have focused on systems with infinite Zeeman energy. Here,
we derive analytically a sweet spot condition for PMMs in a system with finite
Zeeman energy in the absence of Coulomb interaction. We then consider two
numerical models, one in which ECT and CAR are transmitted via superconducting
bulk states and one in which they are transmitted via an Andreev bound state.
In both models we find numerically near zero-energy states that are highly
localized, even in the presence of finite Coulomb interaction. These states can
be related to the analytic sweet spot derived in this work. However, we also
find that in these more realistic models such states do not perfectly satisfy
the characteristics of PMMs, rather they exist only within a "region of
threshold" where PMM characteristics are approximately achieved.
