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Quantum well exciton-polariton light emitting diode

机译:量子阱激子-极化子发光二极管

摘要

A light emitting device made of semiconducting materials. The device has an optical microcavity which supports a resonant mode of predetermined photon energy. Within the cavity is a quantum well of predetermined thickness and energy depth. The quantum well is designed such that it forms bound electron, exciton, lower polariton, and hole energy states of predetermined energy. The energy of an exciton state is set to equal the predetermined photon energy of the microcavity mode such that polariton states are created. A means is provided for resonantly tunneling electrons into a quantum well energy state. In a first embodiment, electrons resonantly tunnel into an electron energy state. In a second embodiment, electrons resonantly tunnel into an exciton energy state, during which tunneling the electrons simultaneously fuse with holes to form excitons. In the first embodiment, the electron state to lower polariton state transition energy is made equal to the energy of a longitudinal optical (LO) phonon of the quantum well material. This energy equivalence facilitates the rapid thermalization of resonantly tunneled electrons to combine with holes and form polaritons resonant with the cavity mode. Thermalization is rapid because it only requires the scattering of a single LO phonon. The photon component of the polariton is then emitted through the leaky cavity reflector. The second embodiment sets the exciton to polariton transition energy equal to the LO phonon energy to facilitate rapid thermalization to the polariton state. Photons are then emitted through the leaky Bragg reflector in the same manner as the first embodiment.
机译:由半导体材料制成的发光器件。该装置具有支持预定光子能量的共振模式的光学微腔。腔体内是具有预定厚度和能量深度的量子阱。量子阱被设计为使得其形成具有预定能量的束缚电子,激子,低极化子和空穴能态。激子态的能量被设置为等于微腔模式的预定光子能量,从而产生了极化子态。提供了一种用于将电子谐振地隧穿为量子阱能态的装置。在第一实施例中,电子共振地隧穿成电子能态。在第二实施例中,电子共振地隧穿为激子能态,在此期间电子同时与空穴融合以形成激子。在第一实施例中,使电子态到低极化子态的跃迁能量等于量子阱材料的纵向光学(LO)声子的能量。这种能量等效性促进了共振隧穿电子的快速热化,从而与空穴结合并形成与腔模共振的极化子。热化是快速的,因为它仅需要散射单个LO声子。然后,极化子的光子分量通过泄漏腔反射器发射。第二实施例将激子到极化子跃迁能量设置为等于LO声子能量,以促进快速热化到极化子状态。然后以与第一实施例相同的方式通过泄漏的布拉格反射器发射光子。

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