Spin conduction in anisotropic three-dimensional topological insulators

When topological insulators possess rotational symmetry their spin lifetime is tied to the scattering time. We show that in anisotropic topological insulators this tie can be broken and the spin lifetime can be very large. Two different mechanisms can obtain spin conduction over long distances. The first is tuning the Hamiltonian to conserve a spin operator cosφσ _x+sinφσ _y, while the second is tuning the Fermi energy to be near a local extremum of the energy dispersion. Both mechanisms can produce persistent spin helices. We report spin lifetimes and spin diffusion equations.