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Doping-dependent evolution of low-energy excitations and quantum phase transitions within an effective model for high-T-c copper oxides

机译:高T-c氧化铜有效模型中低能激发和量子相变的掺杂依赖性演化

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In this paper a mean-field theory for the spin-liquid paramagnetic non-superconducting phase of the p- and n-type high-T-c cuprates is developed. This theory applied to the effective t-t'-t ''-J* model with the ab initio calculated parameters and with the three-site correlated hoppings. The static spin-spin and kinematic correlation functions beyond Hubbard-I approximation are calculated self-consistently. The evolution of the Fermi surface and band dispersion is obtained for the wide range of doping concentrations x. For p-type systems the three different types of behavior are found and the transitions between these types are accompanied by the changes in the Fermi surface topology. Thus a quantum phase transitions take place at x = 0.15 and at x = 0.23.Due to the different Fermi surface topology we found for n-type cuprates only one quantum critical concentration, x = 0.2. The calculated doping dependence of the nodal Fermi velocity and the effective mass are in good agreement with the experimental data.
机译:本文针对p型和n型高T-c铜酸盐的自旋液体顺磁非超导相建立了平均场理论。该理论适用于有效的t-t'-t''-J *模型,该模型具有从头算起的参数和三点相关的跳跃。自洽地计算了超出Hubbard-I近似的静态自旋和运动相关函数。对于宽范围的掺杂浓度x,可以获得费米表面和能带色散的演变。对于p型系统,发现了三种不同类型的行为,这些类型之间的过渡伴随着费米表面拓扑的变化。因此,量子相变发生在x = 0.15和x = 0.23处。由于费米表面拓扑的不同,我们发现n型铜酸盐仅具有一个量子临界浓度x = 0.2。计算的节点费米速度和有效质量的掺杂依赖性与实验数据良好吻合。

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