Abstract
The FQHE was realized in high-mobility 2DEG in GaAs/Al x Ga1-x As heterostructures [4.1–6] and in high-mobility Si-MOSFETs [4.7]. It is characterized by the fact that the Hall conductance has plateaus quantized to certain simple fractions v of the unit e 2 / h and at the same places, the longitudinal resistivity shows an almost dissipationless current flow.
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Chakraborty, T., Pietiläinen, P. (1995). Fractional Quantum Hall Effect: Introduction. In: The Quantum Hall Effects. Springer Series in Solid-State Sciences, vol 85. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-79319-6_4
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