2015
DOI: 10.1103/physrevb.92.064304
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Incoherent excitation and switching of spin states in exciton-polariton condensates

Abstract: We investigate, theoretically and numerically, the spin dynamics of a two-component excitonpolariton condensate created and sustained by non-resonant spin-polarized optical pumping of a semiconductor microcavity. Using the open-dissipative mean-field model, we show that the existence of well defined phase-locked steady states of the condensate may lead to efficient switching and control of spin (polarization) states with a non-resonant excitation. Spatially inhomogeneous pulsed excitations can cause symmetry b… Show more

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Cited by 21 publications
(29 citation statements)
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“…With a linearly-polarized pump we have an equal probability of creating a spin-up or spin-down condensate. Although the pump laser is nonresonant with the final polariton states, the initially created carrier spin is not entirely randomized during their multiple carrier-carrier and excitonphonon scatterings [5,28,39,40]. As a result of this incomplete spin relaxation of the excited carriers, changing the ellipticity of the pump breaks the symmetry of the condensate toward the same circular polarization as that of the pump.…”
Section: Spontaneous Buildup Of Circular Polarizationmentioning
confidence: 99%
“…With a linearly-polarized pump we have an equal probability of creating a spin-up or spin-down condensate. Although the pump laser is nonresonant with the final polariton states, the initially created carrier spin is not entirely randomized during their multiple carrier-carrier and excitonphonon scatterings [5,28,39,40]. As a result of this incomplete spin relaxation of the excited carriers, changing the ellipticity of the pump breaks the symmetry of the condensate toward the same circular polarization as that of the pump.…”
Section: Spontaneous Buildup Of Circular Polarizationmentioning
confidence: 99%
“…Note that in realistic situations, the spin relaxation time of the reservoir is typically finite (see, e.g., Ref. [47]), which can be accounted with a reservoir model in terms of occupations of the left-and right-circular polarized components [41,42] rather than the total density. The dynamics of the polariton condensate can be described by the driven-dissipative two-component Gross-Pitaevskii equation [41,42,45,48], i.e.,…”
Section: Modelmentioning
confidence: 99%
“…We note that our model assumes a spin-independent reservoir resulting from rapid spin relaxation, hence excludes the polarization transfer from the spin-polarized pump to the condensate as discussed in Refs. [41,42] using spin-polarized reservoir models. Moreover, the spontaneous creation of an elliptically polarized condensate in this work is induced by an interplay between interaction effects and linear polarization energy splitting, and occurs for η > 1 which is beyond the typical experimental regime at present.…”
Section: Introductionmentioning
confidence: 99%
“…[22], we use a nonresonant excitation scheme to ensure that the original coherence of the laser is lost in the relaxation process 25 . We create a polariton condensate with a pseudospin orientation defined by the polarization of the excitation beam 39,40 . As the condensate expands, polaritons propagate over macroscopic distances, whilst their pseudospin collectively precesses.…”
Section: Introductionmentioning
confidence: 99%