  We theoretically study a spin-orbit-coupled nanowire proximitized by a
superconductor in the presence of an externally applied Zeeman field ("Majorana
nanowire") with zero-energy Majorana bound states localized at the two ends of
the wire when the Zeeman spin splitting is large enough for the system to enter
the topological phase. The specific physics of interest in the current work is
the effect of having several tunnel probes attached to the wire along its
length. Such tunnel probes should allow, as a matter of principle, one to
observe both the predicted bulk superconducting gap closing and opening
associated with the topological quantum phase transition as well as the
Majorana bound states at the wire ends showing up as zero-bias conductance
peaks, depending on which probes are used for the tunneling spectroscopy
measurement. Because of the possible invasive nature of the tunnel probes,
producing local potential fluctuations in the nanowire, we find the physical
situation to be quite complex. In particular, depending on the details of the
tunnel barrier operational at the probes, the Majorana nanowire could manifest
additional low-energy Andreev bound states which will manifest their own
almost-zero-bias peaks, complicating the interpretation of the tunneling data
in multiprobe Majorana nanowires. We use two complementary microscopic models
to simulate the probes, finding that the tunneling conductance spectrum depends
rather sensitively on the details of the tunnel barriers at the probes. We
apply our general analysis to simulate a recent multiprobe nanowire experiment
commenting on the nature of the quasiparticle gaps likely controlling the
experimental observations.
