Figure 4: Spin character of the metallic band.
From: Valley spin polarization by using the extraordinary Rashba effect on silicon

SARPES spectra measured along the ky direction around (a) the point and (b) the
point, and (c) along the kx direction around the
point. The directions of the wave vectors kx and ky are shown in Figure 3b. The red (blue) spectra represent the spin pointing to positive (negative) z as indicated in the inset. (d) Schematic illustration of the spin-polarized surface states at
and
. The green (purple) hexagon represents the SBZ. The position of the SBZ is here used to indicate the Fermi level at a coverage of 1.12 (1.01) ML. Illustrations of scattering processes (e) without and (f) with spin flipping. ki is the wave vector of the incident electrons, and k1 and k2 are the wave vectors of the scattered ones. q1 and q2 (q2′) are the intravalley and intervalley scattering wave vectors. (g) A 41.7 × 41.7 nm2 STM image of a Si(111) surface with 1.01 ML of adsorbed Tl. Vsample and tunneling current are +1.0 V and 3.0 nA, respectively. (h) Two-dimensional FFT map of an STM topography obtained for a sample with <0.0005 ML of extra Tl at a Vsample of +0.25 V. The inset in h is the 30 × 30 nm2 STM topography. q space maps of scattering amplitudes obtained from FFT of dI/dV maps at Vsample of (i) +0.5 V and (j) +0.25 V. The insets in i and j are the quasiparticle interference patterns of 30 × 30 nm2 images.