Fig. 5: Multi-atom QPI analysis sampled by sublattice.
From: Interplay of hidden orbital order and superconductivity in CeCoIn5
a, e Topography of the surface of CeCoIn5. (setpoint: V = -10 meV,I = 800 pA). b, f Differential conductance map \({g}\left({{{{{\bf{q}}}}}},E\right)\) of the surface of CeCoIn5. The scattering centers at sublattice a (a, b) and sublattice b (e, f) are marked by red circles, which are involved in the multi-atom analysis. c,g, Simultaneous MA-averaged differential conductance map \({g}_{{MA}}({{{{{\bf{r}}}}}},E)\) at \(E \sim 0\) around the defects at sublattice a (c) and sublattice b (g). d, h Real components of Fourier transformed MA-averaged differential conductance map \({{{{{\rm{Re}}}}}}({g}_{{MA}}\left({{{{{\bf{q}}}}}},E\right))\) at \(E \sim 0\) around the defects at sublattice a (d) and sublattice b (h).
