The fractional quantum Hall effect (FQHE) is a phenomenon observed in two-dimensional electron systems subjected to low temperatures and strong magnetic fields, where the Hall conductance takes on fractional values of the fundamental constant $e^2/h$. This effect signifies the emergence of new states of matter, characterized by collective behavior of electrons, leading to quantized excitations and the formation of anyons, which are neither bosons nor fermions. The FQHE has deep implications for understanding quantum mechanics and topological phases of matter.
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