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Microwave impedance of a dc-biased Josephson Fluxonic Diode in the presence of magnetic field and rf drive

机译:直流偏置约瑟夫森磁通二极管的微波阻抗   存在磁场和射频驱动器

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摘要

The dependence of microwave impedance of a dc-biased Josephson Fluxonic Diode(JFD) under application of both dc magnetic field and rf excitation iscalculated with a variety of conditions. For finite length of a JFD excited bya very low microwave excitation below its plasma frequency, applied dc magneticfield increases the rate of Vortex and Anti-Vortex (VAV) pair generation whichfine-tunes the microwave resistance up to several factors more than its zerofield microwave resistance (R0). Under this circumstance, adding a dc bias formoving VAVs causes oscillation-like features in microwave impedance of JFDeither in forward or reverse bias. As a result, the microwave resistanceincreases up to 30R0 in the forward bias despite the fact that dampingparameter (\b{eta}) can limit this increase. On the other hand, sharp phaseslips are seen in reverse bias mode on the reactance of overdamped JFD whileincreasing the frequency or amplitude of microwave excitation leads tounprecedented effects of resistance which is described.
机译:在多种条件下,计算了直流偏置和射频激励下直流偏置约瑟夫森二极管的微波阻抗依赖性。对于通过低于其等离子体频率的极低微波激发而激发的JFD的有限长度,施加的直流磁场会增加涡旋和反涡旋(VAV)对的产生速率,从而将微波电阻微调至比零场微波电阻更大的几个因素(R0)。在这种情况下,增加用于移动VAV的直流偏置会在JFD的微波阻抗中产生正向或反向偏置中的类似振荡的特征。结果,尽管阻尼参数(\ b {eta})可以限制这种增加,但在正向偏压下,微波电阻仍可增加到30R0。另一方面,在反向偏置模式下,对过阻尼的JFD的电抗可以看到尖锐的相移,同时增加微波激励的频率或幅度会导致前所未有的电阻效应,这已描述。

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