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Strongly interacting photons in quantum dot cavity-QED

机译:量子点腔QED中的强相互作用光子

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A long-standing goal in the field of semiconductor cavity quantum electrodynamics (QED) is the demonstration of photon blockade, where strong optical nonlinearities induce quantum correlations between successive photon emission events [1,2]. In the strong coupling regime of cavity QED the two-level quantum-emitter mediated strong photon-photon interactions ensure that the presence of one photon in the cavity blocks the capture of a second one. Here, we show unmistakable signatures of photon blockade in a strongly coupled single-quantum dot (QD) cavity system by demonstrating anti-bunching of photons upon pulsed resonant excitation of the lowest energy polariton state. When we tune the laser into two-photon resonance with the higher-lying polariton states, we observe strong bunching [3].
机译:半导体腔量子电动力学(QED)领域的一个长期目标是光子阻挡的演示,其中强大的光学非线性引起连续光子发射事件之间的量子相关性[1,2]。在腔QED的强耦合状态下,两级量子发射体介导的强光子-光子相互作用确保了腔中一个光子的存在会阻止第二个光子的捕获。在这里,我们通过展示最低能量极化子态的脉冲共振激发下的光子反聚束,展示了在强耦合单量子点(QD)腔系统中光子阻断的明确特征。当我们将激光调谐到极化态较高的双光子共振时,我们会观察到强烈的聚束[3]。

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