Abstract
Since the first discovery in 1986 by J.G. Bednorz and K.A. Müller [1] of a superconductivity at about 30 K in the cuprate (La,Ba)2CuO4, a incredible amount of work has been carried out in order to establish and understand the fascinating properties of the new “high-TC” superconductors. Very rapidly, it has been shown that conventional electron-phonon couplings could not be the only origin for the high-TC superconductivity (HTSC) and that the electronelectron interactions were fundamental in explaining the “strange metal” properties of the new materials, giving rise for some of them to a clear non-Fermi-liquid behavior (for a comprehensive description of both the experimental and theoretical situations, see for example the review article by A. Kampf [2]). It is now well accepted that the low energy properties of high-TC cuprates are essentially determined by the charge and spin dynamics within the CuO2 layers. As early recognized, the existence of layered crystallographic structures build from a sequence of CuO2 layers separated by block layers playing the role of charge reservoirs is at the origin of the charge transfer mechanism upon doping. Based on experimental as well as theoretical results, a generic phase diagram of High-TC cuprates (shown in Figure 1) has been established.
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Regnault, L.P., Bourges, P., Burlet, P. (1998). Phase Diagrams and Spin Correlations in YBa2Cu3O6+x . In: Furrer, A. (eds) Neutron Scattering in Layered Copper-Oxide Superconductors. Physics and Chemistry of Materials with Low-Dimensional Structures, vol 20. Springer, Dordrecht. https://doi.org/10.1007/978-94-015-1284-8_3
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