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自旋涨落诱导的金属 kagome 晶格配对对称性。

Spin-fluctuation-mediated pairing symmetry on the metallic kagome lattice.

机构信息

Department of Physics and National Laboratory of Solid State Microstructures, Nanjing University, Nanjing 210093, People's Republic of China.

出版信息

J Phys Condens Matter. 2011 May 4;23(17):175702. doi: 10.1088/0953-8984/23/17/175702. Epub 2011 Apr 12.

Abstract

We study the magnetic properties and the superconducting pairing mediated by spin fluctuations on the metallic kagome lattice by using the Hubbard model and the fluctuation exchange approximation. It is found that the spin susceptibility is caused by the nesting of the renormalized Fermi surface. We point out that superconductivity will be favored in the spin-singlet channel and may be more easily realized around 25% hole doping. We find an evolution of the pairing state from a d-wave-like symmetry, described by the E(2g) representation of the group D(6h) at low dopings, to that described by the A(2g) representation at heavy hole dopings.

摘要

我们通过 Hubbard 模型和涨落交换近似研究了金属 kagome 晶格上的自旋涨落介导的磁性质和超导配对。结果发现,自旋磁化率是由重整化费米面的嵌套引起的。我们指出,超导配对将在自旋单重态通道中更有利,并且可能更容易在 25%的空穴掺杂下实现。我们发现配对态从低掺杂时由 D(6h)群的 E(2g)表示描述的类似 d 波对称态演变为重空穴掺杂时由 A(2g)表示描述的状态。

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