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. 2017 Jan 31;8:14216. doi: 10.1038/ncomms14216

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Copyright © 2017, The Author(s)

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(a) ARPES data measured at different emission angles. (b,c) Spin-resolved energy distribution curves (EDCs) for the in-plane tangential direction at emission angles of 8° and −8°, respectively. The error bars indicate the statistical fluctuation in determining the spin polarizations (proportional to where N is the photoemission intensity). (d) Spin-resolved EDCs for the in-plane tangential direction at emission angle of 22°. (e) Spin-resolved EDCs along the out-of-plane direction at emission angle of 8°. (f,g) Spin-resolved EDCs for the radial direction at emission angles of 8° and −8°, respectively. (h) Overview of the spin texture of monolayer PtSe₂ from spin-ARPES measurements.

Inline graphic — (a) ARPES data measured at different emission angles. (b,c) Spin-resolved energy distribution curves (EDCs) for the in-plane tangential direction at emission angles of 8° and −8°, respectively. The error bars indicate the statistical fluctuation in determining the spin polarizations (proportional to where N is the photoemission intensity). (d) Spin-resolved EDCs for the in-plane tangential direction at emission angle of 22°. (e) Spin-resolved EDCs along the out-of-plane direction at emission angle of 8°. (f,g) Spin-resolved EDCs for the radial direction at emission angles of 8° and −8°, respectively. (h) Overview of the spin texture of monolayer PtSe₂ from spin-ARPES measurements.