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Theory of Thermal Conductivity in High-Tc Superconductors below Tc: Comparison between Hole-Doped and Electron-Doped Systems

机译:Tc以下高温超导体的导热系数理论:   空穴掺杂和电子掺杂系统的比较

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摘要

In hole-doped high-Tc superconductors, thermal conductivity increasesdrastically just below Tc, which has been considered as a hallmark of a nodalgap. In contrast, such a coherence peak in thermal conductivity is not visiblein electron-doped compounds, which may indicate a full-gap state such as a(d+is)-wave state. To settle this problem, we study the thermal conductivity inthe Hubbard model using the fluctuation-exchange (FLEX) approximation, whichpredicts that the nodal d-wave state is realized in both hole-doped andelectron-doped compounds. The contrasting behavior of thermal conductivity inboth compounds originates from the differences in the hot/cold spot structure.In general, a prominent coherence peak in thermal conductivity appears inline-node superconductors only when the cold spot exists on the nodal line.
机译:在掺杂空穴的高Tc超导体中,热导率仅在Tc以下急剧增加,这被认为是节点间隙的标志。相反,这种热导率的相干峰在掺杂电子的化合物中不可见,这可能表示全能隙状态,例如a(d + is)波状态。为了解决这个问题,我们使用涨落交换(FLEX)近似方法在Hubbard模型中研究了导热系数,该系数可以预测在空穴掺杂和电子掺杂化合物中都实现了节点d波状态。两种化合物的热导率的对比行为均来自于热/冷点结构的差异。通常,只有当节点上存在冷点时,热导率的显着相干峰才会出现在节点内超导体中。

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  • 年度 2007
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  • 正文语种 {"code":"en","name":"English","id":9}
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