Abstract

Hidden Rashba and Dresselhaus spin splittings in centrosymmetric crystals with subunits/sectors having non-centrosymmetric symmetries (the R-2 and D-2 effects) have been predicted theoretically and then observed experimentally, but the microscopic mechanism remains unclear. Here we demonstrate that the spin splitting in the R-2 effect is enforced by specific symmetries, such as non-symmorphic symmetry in the present example, which ensures that the pertinent spin wavefunctions segregate spatially on just one of the two inversion-partner sectors and thus avoid compensation. We further show that the effective Hamiltonian for the conventional Rashba (R-1) effect is also applicable for the R-2 effect, but applying a symmetry-breaking electric field to a R-2 compound produces a different spin-splitting pattern than applying a field to a trivial, non-R-2, centrosymmetric compound. This finding establishes a common fundamental source for the R-1 effect and the R-2 effect, both originating from local sector symmetries rather than from the global crystal symmetry per se.

Highlights

  • Hidden Rashba and Dresselhaus spin splittings in centrosymmetric crystals with subunits/ sectors having non-centrosymmetric symmetries have been predicted theoretically and observed experimentally, but the microscopic mechanism remains unclear

  • Centrosymmetric systems are supposed to lack these effects, there is a large class of systems whose global crystal symmetry (GCS) is centrosymmetric, but they consist of individual sectors with noncentrosymmetric local sector symmetry (LSS)

  • One might naively think that the observed R-2 spin splitting is due to inadvertent breaking of the inversion symmetry in an ordinary centrosymmetric compound.[21]

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Summary

Introduction

Hidden Rashba and Dresselhaus spin splittings in centrosymmetric crystals with subunits/ sectors having non-centrosymmetric symmetries (the R-2 and D-2 effects) have been predicted theoretically and observed experimentally, but the microscopic mechanism remains unclear. ATmheutse,rtαhRe large R-2 effect along this BZ direction originates from wavefunction segregation on each of the two inversion-partner sectors, avoiding mutual compensation of local dipolar electric fields.

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