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arXiv 0705.2239cond-mat.supr-con
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高温超导体中约瑟夫森涡旋晶格的电动力学

Electrodynamics of Josephson vortex lattice in high-temperature superconductors

A. E. Koshelev

摘要:

研究了层状超导体中约瑟夫森涡旋晶格对高频c轴电场的响应。我们发现了一个简单的关系连接的动态介电常数与超导相的扰动,引起振荡电场。数值求解方程的振荡相,我们计算了在不同的磁场的损失函数的频率依赖性,包括区域的稀释和密集的约瑟夫森涡旋晶格。整体行为主要由c轴和面内耗散参数决定,这与各向异性成反比。在$\mathrm{Bi_{2}Sr_{2}CaCu_{2}O_{x}}$和欠掺杂的$\mathrm{YBa_{2}Cu_{3} O_{x}}$中相应地实现了弱耗散和强耗散的情况。响应的主要特征是约瑟夫森等离子体共振峰。在弱耗散的情况下,额外的卫星出现在稀制度主要是在较高的频率区域,由于激发的等离子体模式与波矢量设置的晶格结构。在密格极限下,等离子体峰向高频移动,强度迅速下降,与实验和理论分析一致。涡振荡的唯象理论很好地描述了低频损失函数的行为。在非常强的面内耗散的情况下,在损失函数中的附加峰出现在等离子体频率以下。在欠掺杂的$\mathrm{YBa_{2}Cu_{3} O_{x}}$中实验观察到这样的峰。它是由频率依赖性的面内贡献的损失,而不是一个明确的模式的相位振荡。

英文摘要:

We studied response of the Josephson vortex lattice in layered superconductors to the high-frequency c-axis electric field. We found a simple relation connecting the dynamic dielectric constant with the perturbation of the superconducting phase, induced by oscillating electric field. Numerically solving equations for the oscillating phases, we computed the frequency dependences of the loss function at different magnetic fields, including regions of both dilute and dense Josephson vortex lattices. The overall behavior is mainly determined by the c-axis and in-plane dissipation parameters, which is inversely proportional to the anisotropy. The cases of weak and strong dissipation are realized in $\mathrm{Bi_{2}Sr_{2}CaCu_{2}O_{x}}$ and underdoped $\mathrm{YBa_{2}Cu_{3} O_{x}}$ correspondingly. The main feature of the response is the Josephson-plasma-resonance peak. In the weak-dissipation case additional satellites appear in the dilute regime mostly in the higher-frequency region due to excitation of the plasma modes with the wave vectors set by the lattice structure. In the dense-lattice limit the plasma peak moves to higher frequency and its intensity rapidly decreases, in agreement with experiment and analytical theory. Behavior of the loss function at low frequencies is well described by the phenomenological theory of vortex oscillations. In the case of very strong in-plane dissipation an additional peak in the loss function appears below the plasma frequency. Such peak has been observed experimentally in underdoped $\mathrm{YBa_{2}Cu_{3} O_{x}}$. It is caused by frequency dependence of in-plane contribution to losses rather then a definite mode of phase oscillations.

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