Spin Response to Localized Pumps: Exciton Polaritons Versus Electrons and Holes

TL;DR

This paper compares spin transport and response patterns of polaritons, electrons, and holes under localized pumping, revealing distinctive spatial and magnetic field-dependent behaviors useful for spintronic device design.

Contribution

It provides a comparative analysis of spin responses for polaritons, electrons, and holes in diffusive regimes with localized pumps, highlighting differences in spatial patterns and magnetic field responses.

Findings

Distinct spin patterns for each particle type under localized pumps

Differences in spatial multipole character and magnetic field resonances

Potential applications in designing spintronic systems and measuring spin-orbit interactions

Abstract

Polariton polarization can be described in terms of a pseudospin which can be oriented along the $x,\,y,$ or $z$ axis, similarly to electron and hole spin. Unlike electrons and holes where time-reversal symmetry requires that the spin-orbit interaction be odd in the momentum, the analogue of the spin-orbit interaction for polaritons, the so-called TE-TM splitting, is even in the momentum. We calculate and compare spin transport of polariton, electron, and hole systems, in the diffusive regime of many scatterings. After dimensional rescaling diffusive systems with spatially uniform particle densities have identical dynamics, regardless of the particle type. Differences between the three particles appear in spatially non-uniform systems, with pumps at a specific localized point. We consider both oscillating pumps and transient (delta-function) pumps. In such systems each particle type produces distinctive spin patterns. The particles can be distinguished by their differing spatial multipole character, their response and resonances in a perpendicular magnetic field, and their relative magnitude which is largest for electrons and weakest for holes. These patterns are manifested both in response to unpolarized pumps which produce in-plane and perpendicular spin signals, and to polarized pumps where the spin precesses from in-plane to out-of-plane and vice versa. These results will be useful for designing systems with large spin polarization signals, for identifying the dominant spin-orbit interaction and measuring subdominant terms in experimental devices, and for measuring the scattering time and the spin-orbit coupling's magnitude.