Fig. 2: Large-scale electronic structure.
From: Plethora of tunable Weyl fermions in kagome magnet Fe3Sn2 thin films

a Typical STM topograph of a large flat region of the Fe3Sn surface. Inset in (a) shows Fourier transform of a normalized dI/dV(r, V) map ((dI/dV)/(I/V)) for bias V = −150 mV. Atomic Bragg peaks related to the ab-plane lattice vectors are circled in red. b dI/dV linecut acquired over the vertical line denoted in the STM topograph in the inset. Blue arrow labeled as E0 denotes an abrupt increase in conductance identified as a partial flat band in ref. 28 c Radially averaged linecut generated from the FTs of normalized dI/dV(r, V) maps ((dI/dV)/(I/V)). E0 denotes the energy below which the magnitude of the QPI wave vector is notably enhanced, concomitant with the increase in conductance in (b). Inset in c shows experimentally determined E0 for two film thicknesses extracted from the equivalent radially averaged linecuts as shown in c. STM setup conditions: a Iset = 96 pA, Vsample = 12 mV; inset in a–c Iset = 1 nA, Vsample = 300 mV, Vexc = 5 mV.