Extended Data Fig. 9: Full local and non-local conductance matrix measurements.
From: Observation of edge and bulk states in a three-site Kitaev chain

The main text focuses on measurements of local conductances probed through each of the three normal contacts. For such measurements, the non-local responses are recorded in addition, not shown due to size constraints. Here two measurements are highlighted, for the charge configuration shown in Extended Data Fig. 4g. a. Local and non-local conductances when detuning VQDM, compared to b. numerical simulations of detuning μM. Strikingly, the ZBPs do not appear in the non-local measurements, as expected due to arising from MBSs localised on the outer QDs. Additionally, the same patterns of positive and negative non-local conductance in GML and GLM are observed, with the sign inverting at μ = 0. Unlike the simulations, signals appear in GRM, GLR, GRL and GRM that are not captured by the effective model. We note that a more complete model incorporating explicitly the hybrid regions such as in30 may be needed to fully describe all non-local effects. c. Local and non-local conductances when simultaneously detuning VQDL, VQDM and VQDR, compared to d. numerical simulations of detuning all μi.