Fig. 2: ARPES spectra of the cleaved (001) planes of Bi4(Br1-xIx)4 crystals. | Nature Communications

Fig. 2: ARPES spectra of the cleaved (001) planes of Bi4(Br1-xIx)4 crystals.

From: Coalescence of multiple topological orders in quasi-one-dimensional bismuth halide chains

Fig. 2

a E-kx-ky dispersion spectra measured at the in-situ-cleaved (001) surfaces of Bi4(Br1-xIx)4 crystals with x ranging from 0 to 1(from left to right). The (001) projected time-reversal-invariant (TRI) momenta at the \(\bar{{{{\rm{M}}}}}\) point and the \(\bar{\Gamma }\) point are labeled by a blue dot and a red dot, respectively. The inset shows a schematic diagram of the experimental setup for the (001) surface. b The E-ky dispersion at \(\bar{{{{\rm{M}}}}}\) along the chain direction. The edge-to-edge gap of bulk bands is indicated by the white dashed lines, where the bulk gap firstly shrinks, and then reopens with a transition point around x ~ 0.7. c Energy distribution curves (EDCs) of the corresponding spectra in panel b. The EDCs of ky = 0 are marked in red. The blue and red dots are obtained by the peak fitting of EDCs according to the Lorentz-type distribution equation (see Supplementary Note 4 for details), indicating the half-maximum edge locations of the valence band and the conduction band, respectively. The bottom arrow is used to indicate the trend for the I content in different crystals.

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