论文标题
约瑟夫森的耗散效应在耦合纳米层
Dissipative Josephson effect in coupled nanolasers
论文作者
论文摘要
约瑟夫森效应通常在量子系统中进行研究,在量子系统中,可以忽略耗散或噪声或不发挥关键作用。相比之下,我们在这里讨论了一个设置,其中耗散相互作用确实会放大光子约瑟夫森电流,从而为量子光学干涉学设备的耗散增强灵敏度打开了门口。特别是,我们研究了两种经过相干驱动器的耦合纳米射击器,并通过相干的光子隧穿过程结合。我们通过Fokker-Planck方程来描述该系统,并表明它表现出有趣的非平衡相图,这是纳米层之间相干耦合的函数。随着我们增加该耦合,我们发现相锁和非相锁定的稳态之间的非平衡相变,其中相干性被光子隧道过程破坏。在连贯的相锁状态下,如果纳米射手之间存在相位差异,则会出现不平衡的光子数量,这是由于竞争局部耗散动力学与约瑟夫森照相电流之间的竞争而出现在稳态中的。后者被放大,以提高大量不连贯的抽水速率,并且还靠近激光相变。我们表明,约瑟夫森光电流可用于测量光相差异。在量子限制中,两个纳米酶干涉仪的精度随光子数的平方而生长,因此,可以通过增加光子的不相干泵送速度来增强光子的光子。
Josephson effects are commonly studied in quantum systems in which dissipation or noise can be neglected or do not play a crucial role. In contrast, here we discuss a setup where dissipative interactions do amplify a photonic Josephson current, opening a doorway to dissipation-enhanced sensitivity of quantum-optical interferometry devices. In particular, we study two coupled nanolasers subjected to phase coherent drivings and coupled by a coherent photon tunneling process. We describe this system by means of a Fokker-Planck equation and show that it exhibits an interesting non-equilibrium phase diagram as a function of the coherent coupling between nanolasers. As we increase that coupling, we find a non-equilibrium phase transition between a phase-locked and a non-phase-locked steady-state, in which phase coherence is destroyed by the photon tunneling process. In the coherent, phase-locked regime, an imbalanced photon number population appears if there is a phase difference between the nanolasers, which appears in the steady-state as a result of the competition between competing local dissipative dynamics and the Josephson photo-current. The latter is amplified for large incoherent pumping rates and it is also enchanced close to the lasing phase transition. We show that the Josephson photocurrent can be used to measure optical phase differences. In the quantum limit, the accuracy of the two nanolaser interferometer grows with the square of the photon number and, thus, it can be enhanced by increasing the rate of incoherent pumping of photons into the nanolasers.