Abstract
There has been considerable progress in understanding the fractional quantum Hall effect (FQHE) since the first observation by TSUI et al. [1] in a two-dimensional electron system of a GaAs/AlGaAs heterostructure. The phenomenon is characterized by formation of a plateau in the Hall resistivity pxy and concurrent vanishing of the diagonal resistivity pxx similar to the (integral) quantum Hall effect [2] except that the filling factor becomes a fractional number p/q, where q is an odd integer and p is an integer prime to q. The fractional filling vactor v is defined by v = Nsh/eB where Ns is the electron number density and eB/h is the degeneracy of a Landau level. The temperature dependence of pxx and pxy observed experimentally at fractional filling suggests to us the existence of a finite energy gap between the ground state and the lowest excited state.
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Wakabayashi, J. (1987). Activation Energies of the Fractional Quantum Hall Effect in GaAs/ AlGaAs Heterostructures. In: Landwehr, G. (eds) High Magnetic Fields in Semiconductor Physics. Springer Series in Solid-State Sciences, vol 71. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-83114-0_24
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DOI: https://doi.org/10.1007/978-3-642-83114-0_24
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