Theory for high-Tc superconductors considering inhomogeneous charge distribution -: art. no. 024502

被引:48
作者
de Mello, EVL [1 ]
Caixeiro, ES [1 ]
González, JL [1 ]
机构
[1] Univ Fed Fluminense, Dept Fis, BR-24210340 Niteroi, RJ, Brazil
关键词
D O I
10.1103/PhysRevB.67.024502
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We propose a general theory for the dependence of the critical and pseudogap temperatures T-c and T-* on the doping concentration for high-T-c oxides, taking into account the charge inhomogeneities in the CuO2 planes. Several recent experiments have revealed that the charge density rho in a given compound (mostly underdoped) is intrinsic inhomogeneous with large spatial variations which leads to a local charge density rho(r). These differences in the local charge concentration yield insulator and metallic regions, either in an intrinsic granular or in a stripe morphology. In the metallic region, the inhomogeneous charge density produces also spatial or local distributions which form Cooper pairs at a local superconducting critical temperatures T-c(r) and zero temperature gap Delta(0)(r). For a given compound, the measured onset of the vanishing gap temperature is identified as the pseudogap temperature, that is, T-*, which is the maximum of all T-c(r). Below T-*, due to the distribution of T-c(r)'s, there are some superconducting regions surrounded by an insulator or a metallic medium. The transition to a coherent superconducting state corresponds to the percolation threshold among the superconducting regions with different T-c(r)'s. The charge inhomogeneities have been studied by recent scanning tunneling microscopy experiments which provided a model for our phenomenological distribution. To make definite calculations and compare with the experimental results, we derive phase diagrams for the Bi2Sr2CaCu2O8+x (Bi2212), La2-xSrxCuO4 (LSCO), and YBa2Cu3O7-y (YBCO) families, with a mean field theory for superconductivity using an extended Hubbard Hamiltonian. We show also that this approach provides insights into several experimental features of high-T-c oxides.
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