  We suggest a way to overcome the obstacles that disorder and high density of
states pose to the creation of unpaired Majorana fermions in one-dimensional
systems. This is achieved by splitting the system into a chain of quantum dots,
which are then tuned to the conditions under which the chain can be viewed as
an effective Kitaev model, so that it is in a robust topological phase with
well-localized Majorana states in the outermost dots. The tuning algorithm that
we develop involves controlling the gate voltages and the superconducting
phases. Resonant Andreev spectroscopy allows us to make the tuning adaptive, so
that each pair of dots may be tuned independently of the other. The calculated
quantized zero bias conductance serves then as a natural proof of the
topological nature of the tuned phase.
