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Quantum theory of the dissipative Josephson parametric amplifier

机译:耗散约瑟夫森参数放大器的量子理论

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Recent research in superconducting quantum circuits operating close to the quantum limit results in the need of a quantum mechanical treatment of losses. Of special interest is the dynamic behaviour of an open quantum system. As an example, a negative-resistance Josephson parametric amplifier is treated. The DC bias voltage is chosen such that a strong interaction between the Josephson junction and the two resonant circuits, the signal and the idler circuit, is achieved. Power exchange occurs between the two considered resonator modes and also between the resonator modes and the DC power supply. Losses in the resonators are modeled by the quantum Langevin method, which describes the losses by coupling the resonators to a heat bath representing a photon gas in thermal equilibrium. The derived dynamic behaviour does not provide signal energy saturation, like classically expected for parametric amplifiers. Introducing a phenomenological multi-photon coupling approach, saturation of the amplified signal is ensured. The time evolution of the signal and noise energy is calculated and numerically evaluated for a specific example in cases of both, the quantum Langevin method with and without the phenomenological multi-photon coupling approach. Copyright (c) 2017 John Wiley & Sons, Ltd.
机译:在接近量子极限工作的超导量子电路方面的最新研究导致需要对损耗进行量子力学处理。特别有趣的是开放量子系统的动力学行为。例如,处理负电阻约瑟夫森参数放大器。选择直流偏置电压,以便在约瑟夫森结和两个谐振电路(信号和惰轮)之间实现强大的相互作用。功率交换发生在两个所考虑的谐振器模式之间以及谐振器模式与直流电源之间。谐振器中的损耗通过量子Langevin方法建模,该方法通过将谐振器耦合到代表热平衡中的光子气体的热浴来描述损耗。派生的动态行为不会提供信号能量饱和,就像参数放大器通常期望的那样。引入现象学的多光子耦合方法,可以确保放大信号的饱和。对于使用和不使用现象学多光子耦合方法的量子朗格文方法,对于特定示例,计算并数值估计了信号和噪声能量的时间演化并对其进行了数值评估。版权所有(c)2017 John Wiley&Sons,Ltd.

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