Theory of spin-Hall transport of heavy holes in semiconductor quantum wells
P. Kleinert, V.V. Bryksin

TL;DR
This paper theoretically investigates the spin-Hall effect of heavy holes in semiconductor quantum wells, concluding that a steady-state spin-Hall current does not exist under DC electric fields when using a proper spin current definition.
Contribution
It provides a revised theoretical analysis showing the absence of steady-state spin-Hall currents in heavy-hole systems with Rashba coupling, contrasting previous results.
Findings
Steady-state spin-Hall current is absent under DC fields.
AC fields can induce a spin-Hall effect in these systems.
Proper spin current definition alters previous conclusions.
Abstract
Based on a proper definition of the spin current, we investigate the spin-Hall effect of heavy holes in narrow quantum wells in the presence of Rashba spin-orbit coupling by using a spin-density matrix approach. In contrast to previous results obtained on the basis of the conventional definition of the spin current, we arrive at the conclusion that an electric-field-induced steady-state spin-Hall current does not exist in both, pure and disordered infinite samples. Only an ac field can induce a spin-Hall effect in such systems.
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