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Spin polarized semimagnetic exciton-polariton condensate in magnetic field

机译:磁场中自旋极化的半磁激子-极化子凝聚

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摘要

Owing to their integer spin, exciton-polaritons in microcavities can be used for observation of non-equilibrium Bose-Einstein condensation in solid state. However, spin-related phenomena of such condensates are difficult to explore due to the relatively small Zeeman effect of standard semiconductor microcavity systems and the strong tendency to sustain an equal population of two spin components, which precludes the observation of condensates with a well defined spin projection along the axis of the system. The enhancement of the Zeeman splitting can be achieved by introducing magnetic ions to the quantum wells, and consequently forming semimagnetic polaritons. In this system, increasing magnetic field can induce polariton condensation at constant excitation power. Here we evidence the spin polarization of a semimagnetic polaritons condensate exhibiting a circularly polarized emission over 95% even in a moderate magnetic field of about 3 T. Furthermore, we show that unlike nonmagnetic polaritons, an increase on excitation power results in an increase of the semimagnetic polaritons condensate spin polarization. These properties open new possibilities for testing theoretically predicted phenomena of spin polarized condensate.
机译:由于它们的整数自旋,微腔中的激子-极化子可用于观察固态的非平衡玻色-爱因斯坦凝聚。但是,由于标准半导体微腔系统的塞曼效应相对较小,并且很容易维持两种自旋组分的均等化趋势,因此难以探索此类冷凝物的自旋相关现象。这使得无法观察到自旋清晰的冷凝物沿系统轴的投影。通过将磁性离子引入量子阱,从而形成半磁性极化子,可以实现塞曼分裂的增强。在此系统中,不断增加的磁场会在恒定激发功率下引起极化子凝聚。在这里,我们证明了即使在大约3 T的中等磁场中,半磁性极化子冷凝物的自旋极化也显示出超过95%的圆极化发射。此外,我们表明,与非磁性极化子不同,激发功率的增加导致磁极化强度的增加。半磁极化子凝结自旋极化。这些特性为测试自旋极化冷凝物的理论预测现象提供了新的可能性。

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