Rojan Katharina, Léger Yoan, Morigi Giovanna, Richard Maxime, Minguzzi Anna
Univ. Grenoble Alpes, CNRS, LPMMC, 38000 Grenoble, France.
Theoretische Physik, Universität des Saarlandes, D-66123 Saarbrücken, Germany.
Phys Rev Lett. 2017 Sep 22;119(12):127401. doi: 10.1103/PhysRevLett.119.127401. Epub 2017 Sep 18.
Semiconductor microcavities in the strong-coupling regime exhibit an energy scale in the terahertz (THz) frequency range, which is fixed by the Rabi splitting between the upper and lower exciton-polariton states. While this range can be tuned by several orders of magnitude using different excitonic media, the transition between both polaritonic states is dipole forbidden. In this work, we show that, in cadmium telluride microcavities, the Rabi-oscillation-driven THz radiation is actually active without the need for any change in the microcavity design. This feature results from the unique resonance condition which is achieved between the Rabi splitting and the phonon-polariton states and leads to a giant enhancement of the second-order nonlinearity.
处于强耦合 regime 的半导体微腔在太赫兹(THz)频率范围内展现出一个能量尺度,该尺度由上下激子 - 极化激元态之间的拉比分裂所确定。虽然使用不同的激子介质可以将这个范围调谐几个数量级,但两个极化激元态之间的跃迁是偶极禁戒的。在这项工作中,我们表明,在碲化镉微腔中,拉比振荡驱动的太赫兹辐射实际上是活跃的,而无需对微腔设计进行任何改变。这一特性源于拉比分裂与声子 - 极化激元态之间实现的独特共振条件,并导致二阶非线性的巨大增强。