Fig. 2: Effective masses and Fermi energies of the hole bands. | Communications Physics

Fig. 2: Effective masses and Fermi energies of the hole bands.

From: Resurgence of superconductivity and the role of dxy hole band in FeSe1−xTex

Fig. 2

The effective masses of the α band in a, the β band in b and the γ hole band in c as a function of Te concentration. The solid lines in a and b are linear fits for each data set at different high symmetry points, Γ (red circles) and Z (blue squares). Data for β are from both polarisations, with open and solid symbols corresponding to linear vertical and linear horizontal, respectively. The solid line in c is a 5th order polynomial fit to the data. Open diamond and triangles are from refs. 31 and30, respectively. The Fermi energies of each band are plotted as a function of x in d (E0,α), e (E0,β) and f (E0,γ), where data from refs. 31 and30 are added. The solid lines in d and e are linear fits, while the solid line in f is described by a phenomenological model detailed in the Discussion. The error bars in all plots are calculated from the covariance values produced within the non-linear least squares fitting function.

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