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arXiv 1005.2437cond-mat.supr-concond-mat.str-el
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铁磷族化合物中的竞争次序和配对态的性质

Competing order and nature of the pairing state in the iron pnictides

Rafael M. Fernandes, Jörg Schmalian

摘要:

我们发现磁性和超导电性之间的竞争可以用来确定铁砷化物的配对状态。为此,我们证明了巡回反铁磁相(AFM)和非常规的$s^{+-}$符号改变超导状态(SC)的边界附近的微观共存和宏观相分离,解释了实验观察到的竞争有序状态。相反,常规的$s^{++}$配对不能与磁性共存。扩展的微观自由能的系统与竞争订单周围的多临界点,我们发现,静态磁性起着内在的带间约瑟夫森耦合的作用,使相图敏感的对称性的库珀对波函数。我们把这个结果与准粒子激发谱和具有粒子-空穴对称性的系统的涌现SO $(5)$对称性联系起来。我们的结果依赖于这样的假设,即形成有序矩的相同电子有助于超导凝聚体,并且该系统接近粒子-空穴对称性。我们还比较了抑制SC在不同区域的FeAs相图,表明,而在欠掺杂侧,这是由于与AFM的竞争,在过掺杂侧,它是有关的消失的口袋从费米表面。

英文摘要:

We show that the competition between magnetism and superconductivity can be used to determine the pairing state in the iron arsenides. To this end we demonstrate that the itinerant antiferromagnetic phase (AFM) and the unconventional $s^{+-}$ sign-changing superconducting state (SC) are near the borderline of microscopic coexistence and macroscopic phase separation, explaining the experimentally observed competition of both ordered states. In contrast, conventional $s^{++}$ pairing is not able to coexist with magnetism. Expanding the microscopic free energy of the system with competing orders around the multicritical point, we find that static magnetism plays the role of an intrinsic interband Josephson coupling, making the phase diagram sensitive to the symmetry of the Cooper pair wavefunction. We relate this result to the quasiparticle excitation spectrum and to the emergent SO$(5)$ symmetry of systems with particle-hole symmetry. Our results rely on the assumption that the same electrons that form the ordered moment contribute to the superconducting condensate and that the system is close to particle-hole symmetry. We also compare the suppression of SC in different regions of the FeAs phase diagram, showing that while in the underdoped side it is due to the competition with AFM, in the overdoped side it is related to the disappearance of pockets from the Fermi surface.

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