Abstract
The discoveries of the integer and fractional quantum Hall effects [1, 2] in the early 1980s opened an exciting field for condensed matter physics. The continuous effort in this area during the past quarter century has been particularly rewarding. The interplay between Landau quantization, disorder, electron-electron and spin interactions gives rise to a large variety of fascinating electronic states [3–6]. Some examples are incompressible quantum fluids with quasi-particles carrying fractional charge [7–11], compressible metallic states composed of composite particles [12– 14], insulating Wigner crystal electron solids [15, 16], Bose-Einstein condensates [17], Skyrmion spin textures in quantum Hall ferromagnets [18, 19], non-Abelian states [20–22], electron liquid crystal phases [23–28], and so forth. Indeed, this list is incomplete.
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Li, Y.Q., Smet, J.H. (2008). Nuclear-Electron Spin Interactions in the Quantum Hall Regime. In: Dyakonov, M.I. (eds) Spin Physics in Semiconductors. Springer Series in Solid-State Sciences, vol 157. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-540-78820-1_12
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