Plaquette Valence Bond Theory of Cuprate High-Temperature Superconductivity

M. Harland, Tim B Berberich, M. Katsnelson, A. Lichtenstein
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Abstract

We investigate the phenomenon of high-temperature superconductivity within a strong coupling perspective. The occurence is traced to a quantum critical point that is in the phase diagram of the plaquette's t; t0-Hubbard model. We develop a bottom-up approach combining several methods, i.e. exact diagonalization of an isolated plaquette, the Lanczos-method for a plaquette within a bath and cluster dynamical Mean-Field theory with continuous time quantum Monte-Carlo solver to embedd the plaquette in a lattice environment. The quantum critical point is located where the N = 2; 3; 4-sectors of the plaquette cross. This point is also found to show optimal doping. The wave order turns out to be largest at the localized-itinerant transition of the electrons. Furthermore, we present an explenation for the pseudo-gap phenomenon, that is explained by a soft mode related to local singlets of the plaquette. The theory presented here is similar to the resonating valence bond theory, but stresses the importance of local singlets.
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铜高温超导的板价键理论
我们从强耦合的角度研究高温超导现象。该事件可追溯到斑块t相图中的量子临界点;t0-Hubbard模型。我们开发了一种自下而上的方法,结合几种方法,即孤立斑块的精确对角化,池内斑块的lanczos方法和簇动力学平均场理论与连续时间量子蒙特卡罗求解器将斑块嵌入晶格环境中。量子临界点位于N = 2处;3;4个扇形十字。这一点也显示了最佳的兴奋剂。在电子的局域流动跃迁处,波阶最大。此外,我们提出了一种伪间隙现象的解释,这是由与斑块局部单重态相关的软模式解释的。这里提出的理论类似于共振价键理论,但强调局部单重态的重要性。
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