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. 2015 Oct 13;6:8595. doi: 10.1038/ncomms9595

Figure 2. Electronic structure of β-PdBi2.

Figure 2

(a) Calculated Fermi surfaces shown with the first Brillouin zone. kx, ky and kz axes for the crystal momentum space are depicted. Γ, Z, N, X and M are the high-symmetry points. The square plane represents the two-dimensional (2D) projected surface Brillouin zone with 2D high-symmetry points, Inline graphic, Inline graphic and Inline graphic. (b) Four-fold symmetrized Fermi surface recorded by angular-resolved photoemission spectroscopy (ARPES). The image is obtained by integrating intensities in the energy window of ±8 meV at the Fermi level. The colour scale indicates the intensity. Two electron-like and two hole-like Fermi surfaces are denoted by α, β and γ, δ, respectively. (c) ARPES image recorded along Inline graphicInline graphic and Inline graphicInline graphic cuts, shown as the light-blue and -green broken lines in b, respectively. The colour scale indicates the intensity. (d) Calculated bulk band dispersions projected onto 2D surface Brillouin zone. Blue (red) curves correspond to kz=0 (2π/c). (e) Surface band dispersions obtained by slab calculation of 11 PdBi2 layers. Orange rectangles in ce indicate the region where the surface Dirac cone appears.