2018
DOI: 10.1103/physrevlett.120.225301
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Optical Bistability under Nonresonant Excitation in Spinor Polariton Condensates

Abstract: We realize bistability in the spinor of polariton condensates under nonresonant optical excitation and in the absence of biasing external fields. Numerical modeling of the system using the Ginzburg-Landau equation with an internal Josephson coupling between the two spin components of the condensate qualitatively describes the experimental observations. We demonstrate that polariton spin bistability strongly depends on the condensate's overlap with the exciton reservoir by tuning the excitation geometry and sam… Show more

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Cited by 51 publications
(37 citation statements)
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“…Therefore, while the previous two models (Refs. [26][27][28] and [12,25]) can separately explain parts of our results successfully, they fail to grasp the full picture.…”
Section: Theory and Simulationsmentioning
confidence: 78%
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“…Therefore, while the previous two models (Refs. [26][27][28] and [12,25]) can separately explain parts of our results successfully, they fail to grasp the full picture.…”
Section: Theory and Simulationsmentioning
confidence: 78%
“…We report on two distinct and unusual effects: spin inversion, which forms condensates with elliptical polarization (spin) of the opposite handedness to that of the nonresonant pump, and spin/intensity bistability with pump power. While such effects were recently reported [26,27], both were attributed to an interplay of linear polarization splitting and spin-asymmetric reservoir nonlinearities within a zero-dimensional model [28]. Studying the dependence of these effects on pump polarization ellipticity and trap size reveals that these two phenomena (1) are strongly trap-size dependent, (2) can only be observed within a certain range of pump ellipticity, (3) can be observed independently from each other, indicating they arise from different physical processes, and (4) are position dependent.…”
Section: Introductionmentioning
confidence: 92%
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“…For example, consider a cavity with a resonance frequency ω 0 = 360 THz, a total loss rate Γ = 10 GHz, and U/Γ = 0.01; these values are typical for III-V semiconductor cavities in Ref. [32,33,43,44]. The calculations in Figs.…”
Section: Sensitivity and Detection Speedmentioning
confidence: 99%