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Phase separation and competition of superconductivity and magnetism in the two-dimensional Hubbard model: From strong to weak coupling

机译:超导电磁相分离与竞争   二维Hubbard模型:从强耦合到弱耦合

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摘要

Cooperation and competition between the antiferromagnetic, d-wavesuperconducting and Mott-insulating states are explored for the two-dimensionalHubbard model including nearest and next-nearest-neighbor hoppings at zerotemperature. Using the variational cluster approach with clusters of differentshapes and sizes up to 10 sites, it is found that the doping-driven transitionfrom a phase with microscopic coexistence of antiferromagnetism andsuperconductivity to a purely superconducting phase is discontinuous for stronginteraction and accompanied by phase separation. At half-filling the system isin an antiferromagnetic Mott-insulating state with vanishing chargecompressibility. Upon decreasing the interaction strength U below a certaincritical value of roughly U=4 (in units of the nearest-neighbor hopping),however, the filling-dependent magnetic transition changes its character andbecomes continuous. Phase separation or, more carefully, the tendency towardsthe formation of inhomogeneous states disappears. This critical value is incontrast to previous studies, where a much larger value was obtained. Moreover,we find that the system at half-filling undergoes the Mott transition from aninsulator to a state with a finite charge compressibility at essentially thesame value. The weakly correlated state at half-filling exhibitssuperconductivity microscopically admixed to the antiferromagnetic order. Thisscenario suggests a close relation between phase separation and theMott-insulator physics.
机译:研究了二维Hubbard模型的反铁磁,d波超导状态和Mott绝缘状态之间的合作与竞争,该二维Hubbard模型包括零温度下的最近和最近邻跳变。使用具有多达10个位点的不同形状和大小的簇的变分簇方法,发现掺杂驱动从具有反铁磁和超导微观共存的相到纯超导相的间断对于强相互作用是不连续的,并伴随有相分离。在半填充时,系统处于反铁磁Mott绝缘状态,电荷压缩性消失。但是,在将相互作用强度U降低到大约U = 4(以最近邻居跳跃为单位)的某个临界值以下时,取决于填充的磁跃迁会改变其特性并变得连续。相分离或更仔细地讲,形成不均匀状态的趋势消失了。该临界值与以前的研究相反,以前的研究获得了更大的值。此外,我们发现半填充系统经历了从绝缘子到具有基本上相同值的有限电荷可压缩性的状态的Mott跃迁。半填充时的弱相关状态在微观上表现出与反铁磁有序混合的超导性。这种情况表明相分离与莫特-绝缘子物理之间存在密切关系。

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