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Plasmon blockade in nanostructured graphene

机译:纳米结构石墨烯中的等离子封锁

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Among the many extraordinary properties of graphene, its optical response allows one to easily tune its interaction with nearby molecules via electrostatic doping. The large confinement displayed by plasmons in graphene nanodisks makes it possible to reach the strong-coupling regime with a nearby quantum emitter, such as a quantum dot or a molecule. In this limit, the quantum emitter can introduce a significant plasmon-plasmon interaction, which gives rise to a plasmon blockade effect. This produces, in turn, strongly nonlinear absorption cross sections and modified statistics of the bosonic plasmon mode. We characterize these phenomena by studying the equal-time second-order correlation function g ~((2))(0), which plunges below a value of 1, thus revealing the existence of nonclassical plasmon states. The plasmon-emitter coupling, and therefore the plasmon blockade, can be efficiently controlled by tuning the doping level of the graphene nanodisks. The proposed system emerges as a new promising platform to realize quantum plasmonic devices capable of commuting optical signals at the single-photon/plasmon level.
机译:在石墨烯的许多非凡特性中,其光学响应使人们可以通过静电掺杂轻松调整其与附近分子的相互作用。等离子体子在石墨烯纳米盘中表现出的较大限制使其可以与附近的量子发射器(例如量子点或分子)达到强耦合状态。在此极限下,量子发射器会引入显着的等离激元-等离激元相互作用,从而产生等离激元阻断效应。反过来,这会产生强非线性吸收截面,并修正了玻色等离子体激元模式。我们通过研究等时二阶相关函数g〜((2))(0)来表征这些现象,该函数跌落到值1以下,从而揭示了非经典等离子体激元状态的存在。通过调节石墨烯纳米盘的掺杂水平,可以有效地控制等离子体激元-发射极的耦合,从而对等离子体激元的阻断。拟议的系统作为实现具有能够在单光子/等离激元水平上交换光信号的量子等离激元设备的新兴平台而出现。

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