Cubic Rashba spin-orbit interaction of two-dimensional hole gas in strained-Ge/SiGe quantum well
arXiv:1408.1148 · doi:10.1103/PhysRevLett.113.086601
Abstract
The spin-orbit interaction (SOI) of the two-dimensional hole gas in the inversion symmetric semiconductor Ge is studied in a strained-Ge/SiGe quantum well structure. We observed weak anti-localization (WAL) in the magnetoconductivity measurement, revealing that the WAL feature can be fully described by the k-cubic Rashba SOI theory. Furthermore, we demonstrated electric field control of the Rashba SOI. Our findings reveal that the heavy hole (HH) in strained-Ge is a purely cubic-Rashba-system, which is consistent with the spin angular momentum mj = +-3/2 nature of the HH wave function.
To be published in Phys. Rev. Lett
References in corpus (6)
- Dissipationless Quantum Spin Current at Room Temperature
- An Exact SU(2) Symmetry and Persistent Spin Helix in a Spin-Orbit Coupled System
- Emergence of the persistent spin helix in semiconductor quantum wells
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Cited by in corpus (5)
- Spontaneous Edge Accumulation of Spin Currents in Finite-Size Two-Dimensional Diffusive Spin-Orbit Coupled SFS Heterostructures
- Long-Range Spin-Triplet Correlations and Edge Spin Currents in Diffusive Spin-Orbit Coupled SNS Hybrids with a Single Spin-Active Interface
- Effective g factor of low-density two-dimensional holes in a Ge quantum well
- Magnetotransport properties of two-dimensional fermions with -cubic Rashba spin-orbit interaction
- Landau quantization, Rashba spin-orbit coupling and Zeeman splitting of two-dimensional heavy holes