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Visualization of optical polarization transfer to photoelectron spin vector emitted from a spin-orbit coupled surface state

Kenta Kuroda1,*,†, Koichiro Yaji2,*,‡, Ryo Noguchi1, Ayumi Harasawa1, Shik Shin1,3, Takeshi Kondo1,4, and Fumio Komori1,§

  • 1Institute for Solid State Physics (ISSP), University of Tokyo, Kashiwa, Chiba 277-8581, Japan
  • 2Research Center for Advanced Measurement and Characterization, National Institute for Materials Science (NIMS), Tsukuba, Ibaraki 305-0003, Japan
  • 3Office of University Professor, The University of Tokyo, Chiba 277-8581, Japan
  • 4Trans-scale Quantum Science Institute, The University of Tokyo, Bunkyo-ku, Tokyo 113-0033, Japan

  • *These authors contributed equally to this work.
  • †Present address: Graduate School of Advanced Science and Engineering, Hiroshima University, 1-3-1 Kagamiyama, Higashi-hiroshima 739-8526, Japan; kuroken224@hiroshima-u.ac.jp
  • ‡YAJI.Koichiro@nims.go.jp
  • §Present address: Institute of Industrial Science, The University of Tokyo, Tokyo 153-8505, Japan.

Phys. Rev. B 105, L121106 – Published 11 March, 2022

DOI: https://doi.org/10.1103/PhysRevB.105.L121106

Abstract

Similar to light polarization that is selected by a superposition of the optical basis, the electron spin direction can be controlled through a superposition of the spin basis. We investigate such a spin interference occurring in the photoemission of a spin-orbit coupled surface state in Bi2Se3 by using spin- and angle-resolved photoemission spectroscopy combined with a laser light source (laser-SARPES). Our laser-SARPES with three-dimensional spin detection and tunable laser polarization including elliptical and circular polarization enables us to directly visualize how the direction of the fully polarized photoelectron spin changes according to the optical phase and orientation of the incident laser polarization. By this advantage of our laser-SARPES, we demonstrate that such optical information can be projected to the three-dimensional spin vector of the photoelectrons. Our results therefore present a spin-polarized electron source permitting us to optically control the pure spin state pointing to an arbitrary direction.

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