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Theory of macroscopic quantum tunneling with Josephson-Leggett collective excitations in multi-band superconducting Josephson junctions

机译:Josephson-Leggett宏观量子隧穿理论   多波段超导约瑟夫森结中的集体激发

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摘要

Collective excitations reveal fundamental properties and potentialapplications of superconducting states. We theoretically study macroscopicquantum tunneling (MQT) in a Josephson junction composed of multi-bandsuperconductors, focusing on a phase mode induced by inter-band fluctuations:the Josephson-Leggett (JL) collective excitation mode. Using the imaginary-timepath-integral method, we derive a formula for the MQT escape rate forlow-temperature switching events. We clarify that the JL mode has two majoreffects on the MQT: (i) the zero-point fluctuations enhance the escape rate,and (ii) the quantum dissipation induced by the couplings to thegauge-invariant phase difference suppresses the quantum tunneling. We show thatthe enhancement exceeds the suppression for a wide range of junctionparameters. This enhancement originates from the single-mode interactionbetween the tunneling variable and the inter-band fluctuations.
机译:集体激发揭示了超导态的基本性质和潜在应用。我们从理论上研究由多频带超导体组成的约瑟夫逊结中的宏观量子隧穿(MQT),重点研究由带间波动引起的相位模式:约瑟夫森-莱格特(JL)集体激发模式。使用虚构的时间路径积分方法,我们得出了针对低温开关事件的MQT逸出率的公式。我们弄清楚JL模式对MQT有两个主要影响:(i)零点波动会提高逸出率,(ii)量规不变相差耦合所引起的量子耗散会抑制量子隧穿。我们显示,对于大范围的结参数,增强作用都超过了抑制作用。这种增强源自隧穿变量和带间波动之间的单模交互作用。

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