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. 2016 Feb 24;7:10829. doi: 10.1038/ncomms10829

Figure 4. Surface g-factor measurement on Sb2Te2Se.

Figure 4

(a) Potential landscape of Sb2Te2Se obtained by mapping E0 at 12 T showing a potential minimum. The centre of the potential minimum is determined by the 2D parabolic potential fitting and marked by a cross. The scale bar corresponds to 10 nm. (b) Tunnelling spectra taken at the potential minimum centre at fields from 3 to 12 T with 1 T intervals. The spectra have been shifted for clarity. (c) E0 values at different B obtained by fitting the data of b with a Lorentz line shape and plotted with black symbols (left axis). The error bars are the standard deviation of the fitting analysis. The effects of the potential and the non-ideal dispersions on the LL0 energies are represented by Inline graphic and Inline graphic, respectively. Their influences can be excluded by subtracting their contributions. The red symbols denote the LL0 energies after subtracting the effect of the potential (E0EV). The blue symbols correspond to the LL0 energies after subtracting the effects from both the potential and the non-ideal dispersions (Inline graphic) (right axis, in the relative energy scale). The black curve denotes the fitting to E0 with B according to equation (2). The red and blue lines represent the linear fitting of E0EV and Inline graphic with B, respectively. (df) Similar data and analysis as ac for a potential maximum of Sb2Te2Se. Measurement conditions of a and d: Vs=215 mV, It=50 pA, Vmod=2.8 mVrms, T=4.4 K and B=12 T. Measurement conditions of b and e: Vs=210 mV, It=50 pA, Vmod=1.8 mVrms and T=4.4 K.