RASHBA-DRESSELHAUS SOC
Spin splitting from broken inversion symmetry
VIEW
OBSERVABLES
k₀ (spin-split shift)—
ΔE (at k_F)—
PSH condition—
Topology—
H_R = α(σ_x k_y - σ_y k_x)
H_D = β(σ_x k_x - σ_y k_y)
Rashba SOC arises from structural inversion asymmetry (e.g., interfaces, gate fields). Dresselhaus from bulk inversion asymmetry (zinc-blende). When α=β, a persistent spin helix emerges — SU(2) symmetry prevents spin relaxation.