Abstract
The history of the quasi two-dimensional (2D) inorganic conductors goes back to approximately 30 years ago, when the transition metal layered dichalcogenides (TMLD) were extensively studied, mostly in relation with their strongly anisotropic anomalous conducting properties [1]. These properties were soon attributed to the Peierls instability induced by special properties of the Fermi surface combined with strong electron-phonon coupling and leading to the so-called charge density wave (CDW) state at low temperature [2, 3]. It was shown later that similar properties are found in some quasi 2D molybdenum bronzes and oxides [4, 5]. More recently, a new family, the monophosphate tungsten bronzes (PO2)4(WO3)2m [6], has provided a model system where the low-dimensional character can be modified without changing the band filling [7]. Meantime, the discovery of superconductivity at high temperature in some copper-based quasi-2D oxides has revived the interest in quasi-2D conducting oxides [8].
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Schlenker, C. (1996). Charge Density Waves in Quasi Two-Dimensional Inorganic Conductors — Molybdenum and Phosphate Tungsten Bronzes. In: Schlenker, C., Dumas, J., Greenblatt, M., van Smaalen, S. (eds) Physics and Chemistry of Low-Dimensional Inorganic Conductors. NATO ASI Series, vol 354. Springer, Boston, MA. https://doi.org/10.1007/978-1-4613-1149-2_8
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