Bi2Sr2CaCu2O8+δ本征结涡旋态层间临界电流

Takashi Yasuda , Tetsuji Uchiyama , Takeshi Fukami , Takafumi Aomine , Shuzo Takano
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引用次数: 1

摘要

我们在平行于c轴的磁场中测量了Bi2Sr2CaCu2O8+δ本征约瑟夫森结的电流-电压(I-V)特性。在涡旋的液相中,I-V曲线呈现出三个阶段:低电流时的欧姆关系、快速电阻转变和准粒子分支。如果在跃迁处定义最大约瑟夫森电流Ic,则其场依赖性与最近对约瑟夫森等离子体频率ωp的测量结果在定量上一致。由此得出结论,Ic和ωp等效地给出了层间相位相干的信息。尽管Josephson电流有限,但在小电流下存在与洛伦兹力无关的耗散,表明液相层间临界电流为零。我们讨论了与涡旋薄煎饼平面内运动有关的相滑移机制的适用性。
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Interlayer Critical Current in the Vortex State of Bi2Sr2CaCu2O8+δ Intrinsic Junctions

We measure the current-voltage (I–V) characteristics of the Bi2Sr2CaCu2O8+δ intrinsic Josephson junctions in the magnetic field parallel to the c-axis. In the liquid phase of vortices, the I–V curve reveals three stages: ohmic relation at low currents, rapid resistive transition and a quasiparticle branch. If the maximum Josephson current Ic is defined at the transition, its field dependence is in quantitative agreement with the recent measurements on the Josephson plasma frequency ωp. This leads to the conclusion that both Ic and ωp equivalently give the information for the interlayer phase coherence. In spite of the finite Josephson current, there appears Lorentz-force-independent dissipation at small currents, indicating that the interlayer critical current is zero in the liquid phase. We discuss the applicability of the phase-slip mechanism associated with the in-plane motion of the vortex pancakes.

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