We develop a theory of the nonlocal conductance $G_{RL}\left(V\right)$ for a disordered Majorana wire tuned near the topological transition critical point. Under these conditions, the antisymmetric part of the differential conductance, $[G_{RL}\left(V\right)-G_{RL}(-V)]/2$, is the dominant one for a sufficiently long wire. This reflects the charge-neutral nature of the critical modes in the wire. We factorize the conductance into a term describing propagation of the critical modes along the wire and terms describing the contacts between the wire and the normal leads. Topological transition affects only the former term. At the critical point, the localization length has a logarithmic singularity at the Fermi level, $l\left(E\right)\propto ln(1/E)$. This singularity directly manifests in the conductance magnitude as $ln|G_{RL}\left(V\right)/G_Q|\sim L/l\left(eV\right)$ for the wire of length $L\gg l\left(eV\right)$. Tuning the wire away from the immediate vicinity of the critical point changes the monotonicity of $l\left(E\right)$. This change in monotonicity allows us to define the width of the critical region around the transition point.

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• Quantum phase transitions
• Topological superconductors
• Disordered systems
• S-matrix method in transport