  We present an approach to the fractional quantum Hall effect observed in
grapheme (GFQHE), basing us on the model developed previously for the
fractional quantum Hall effect in a two-dimensional electron system embedded in
a quantum well (FQHE) [Hidalgo, 2013(*)]. The main idea in the view proposed
f0r the FQHE is the breaking of the symmetry of the Hamiltonian of every
electron in a two-dimensional electron gas (2DEG) under the application of a
magnetic field and in the presence of an electrostatic potential due to the
ionized impurities. As the magnetic field increases the effect of that
electrostatic potential evolves; changing in turn the spatial symmetry of the
Hamiltonian: from continuous to discrete one. The model provides the odd
fractional states, and corresponding plateaux, p/3, p being any integer,
observed in graphene.
