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Mesoscopic fluctuations in biharmonically driven flux qubits

机译:双谐波驱动通量量子比特的介观波动

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摘要

We investigate flux qubits driven by a biharmonic magnetic signal, with aphase lag that acts as an effective time reversal broken parameter. The drivinginduced transition rate between the ground and the excited state of the fluxqubit can be thought as an effective transmitance, profiting from a directanalogy between interference effects at avoided level crossings and scatteringevents in disordered electronic systems. For time scales prior to fullrelaxation but large compared to the decoherence time, this characteristic ratehas been accessed experimentally and its sensitivity with both the phase lagand the dc flux detuning explored. In this way signatures of UniversalConductance Fluctuations-like effects have recently been analized in fluxqubits and compared with a phenomenological model that only accounts fordecoherence, as a classical noise. We here solve the full dynamics of thedriven flux qubit in contact with a quantum bath employing the Floquet MarkovMaster equation. Within this formalism relaxation and decoherence rates resultstrongly dependent on both the phase lag and the dc flux detuning.Consequently, the associated pattern of fluctuations in the characteristicrates display important differences with those obtained within the mentionedphenomenological model. In particular we demonstrate the Weak Localization-likeeffect in the averages values of the relaxation rate. Our predictions can betested for accessible, but longer time scales than the current experimentaltimes.
机译:我们研究了由双谐波磁信号驱动的磁通量子比特,其相位滞后可作为有效的时间反转中断参数。可以从基态和磁通量比特的激发态之间的驱动诱导的跃迁速率视为有效的透射率,这得益于避免电子交叉处的干扰效应和避免杂散电子系统中散射事件的直接相似性。对于完全弛豫之前的时间标度,但与退相干时间相比,该标度较大,已通过实验获得了该特征速率,并探索了其灵敏度与相位滞后和直流通量失谐之间的关系。通过这种方式,最近已经在通量量子比特中分析了类似“通用传导波动”的信号,并将其与仅解释退相干性的现象学模型(作为经典噪声)进行了比较。我们在这里使用Floquet MarkovMaster方程求解与量子浴接触的驱动通量量子位的完整动力学。在这种形式主义下,弛豫和退相干率的结果强烈地取决于相位滞后和直流通量失谐。因此,特征量的相关波动模式与上述现象学模型中获得的波动模式显示出重要的差异。特别地,我们在松弛率的平均值中证明了弱定位效应。可以测试我们的预测的可访问性,但是比当前的实验时间更长的时间范围。

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