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arXiv 1602.03147cond-mat.mes-hallphysics.optics
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超导Sn膜在逾渗上下的微波研究

Microwave study of superconducting Sn films above and below percolation

Manfred H. Beutel, Nikolaj G. Ebensperger, Markus Thiemann, Gabriele Untereiner, Vincent Fritz, Mojtaba Javaheri, Jonathan Nägele, Roland Rösslhuber, Martin Dressel, Marc Scheffler

摘要:

超导Sn膜($T_c \approx$ 3.8 K)的电子性质在将膜厚度减小到几nm时显著改变,特别是接近逾渗阈值。这种Sn样品的低能量电动力学可以通过微波光谱学来探测,例如使用超导带状线谐振器。在这里,我们研究锡薄膜,通过热蒸发沉积-在38 nm和842 nm之间的厚度范围-其中包括渗滤过渡。我们使用超导Pb带线谐振器探测这些Sn薄膜在4GHz和20 GHz之间的频率范围内的微波响应,温度从7.2 K下降到1.5 K。谐振器的测量品质因数随着温度的升高而降低,这是由于损耗增加。作为样品厚度的函数,我们观察到三个制度具有显着不同的性能:低于渗流,即合奏断开超导岛的样品,表现出介电性能与可以忽略不计的损失,表明宏观电流路径所需的可观的动态导电性的锡在GHz频率。作为另一限制,厚Sn膜导致高于和低于Sn的$T_c$的低损耗谐振,如对于体导体所预期的。但在一个中间厚度的制度,上面的渗流和类似的形态的锡,我们观察到一个完全不同的行为:超导状态具有类似的微波响应较厚,完全覆盖的薄膜,微波损耗低,但这些锡膜的金属状态是如此有损谐振器的操作被完全抑制。

英文摘要:

The electronic properties of superconducting Sn films ($T_c \approx$ 3.8 K) change significantly when reducing the film thickness down to a few nm, in particular close to the percolation threshold. The low-energy electrodynamics of such Sn samples can be probed via microwave spectroscopy, e.g. with superconducting stripline resonators. Here we study Sn thin films, deposited via thermal evaporation -ranging in thickness between 38 nm and 842 nm- which encompasses the percolation transition. We use superconducting Pb stripline resonators to probe the microwave response of these Sn films in a frequency range between 4 GHz and 20 GHz at temperatures from 7.2 K down to 1.5 K. The measured quality factor of the resonators decreases with rising temperature due to enhanced losses. As a function of the sample thickness we observe three regimes with significantly different properties: samples below percolation, i.e. ensembles of disconnected superconducting islands, exhibit dielectric properties with negligible losses, demonstrating that macroscopic current paths are required for appreciable dynamical conductivity of Sn at GHz frequencies. Thick Sn films, as the other limit, lead to low-loss resonances both above and below $T_c$ of Sn, as expected for bulk conductors. But in an intermediate thickness regime, just above percolation and with labyrinth-like morphology of the Sn, we observe a quite different behavior: the superconducting state has a microwave response similar to the thicker, completely covering films with low microwave losses; but the metallic state of these Sn films is so lossy that resonator operation is suppressed completely.

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