Fig. 3: Magnetic field response and depth profile of magnetism in SRO214.
From: Unveiling unconventional magnetism at the surface of Sr2RuO4

a, b, Temperature dependence of the local field amplitude Bloc (a) and of the shift in the depolarization rate, Δλ, from the λ value measured at T = 200 K (b) measured in TF with amplitude of the external field Bext = 1500 G at E = 3 keV (red symbols with error bars) and E = 14 keV (blue symbols with error bars). Error bars in (a) are within the symbols. The inset schematic in (a) shows the relative orientation of the applied field Bext with respect to the muon spin polarization Sμ+ in our orthonormal reference-axes system for the TF configuration. The Δλ values in (b) are different from those shown in Fig. 2, as they are measured at a different stage of the experiment after warming the samples to room T, degaussing the magnet and zero-field cooling the samples again before applying Bext. c, d Shift in the local field amplitude ΔBloc (c) and in Δλ (d) between T = 100 K > Ton and T = 5 K < Ton measured in TF as a function of E for Bext = 100 G (green symbols with error bars) and Bext = 1500 G (purple symbols with error bars). The top axes are the corresponding muon average stopping depth \(\bar{z}\) values determined from the simulated muon stopping distributions in Fig. 1d. Dashed lines in (b) to (d) are guides to the eye.