Taking advantage of the two-parameter central extension of the planar Galilei
group, we construct a non relativistic particle model in the plane. Owing to
the extra structure, the coordinates do not commute. Our model can be viewed as
the non-relativistic counterpart of the relativistic anyon considered before by
Jackiw and Nair. For a particle moving in a magnetic field perpendicular to the
plane, the two parameters combine with the magnetic field to provide an
effective mass. For vanishing effective mass the phase space admits a
two-dimensional reduction, which represents the condensation to collective
Hall'' motions and justifies the rule called Peierls substitution’'.
Quantization yields the wave functions proposed by Laughlin to describe the
Fractional Quantum Hall Effect.

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