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Unconventional superconducting symmetry in a checkerboard antiferromagnet studied via renormalized mean-field theory

机译:基于规范化平均场理论研究棋盘格反铁磁体中的非常规超导对称性

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摘要

We use a renormalized mean-field theory to study the Gutzwiller projected Bardeen-Cooper-Schrieffer states of the extended Hubbard model in the large U limit or the t-t'-J-J' model on a two-dimensional checkerboard lattice. At small t'/t, the frustration due to the diagonal terms of t' and J' does not alter the d_(x~2-y~2)-wave pairing symmetry, and the negative (positive) t'/t enhances (suppresses) the pairing order parameter. At large t'/t, the ground state has an s-s wave symmetry. At the intermediate t'/t, the ground state is d+id or d+is wave with time reversal symmetry broken.
机译:我们使用重新归一化的平均场理论来研究大U极限或二维棋盘格上的t-t'-J-J'模型的扩展Hubbard模型的Gutzwiller投影Bardeen-Cooper-Schrieffer状态。在小t'/ t时,由于t'和J'的对角线项而产生的挫败感不会改变d_(x〜2-y〜2)波对对称性,并且负(正)t'/ t增强(禁止)配对顺序参数。在大t / t时,基态具有s-s波对称性。在中间t'/ t处,基态为d + id或d + is波,其中时间反转对称性破裂。

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