The quasicrystalline state of matter and the role of quasiperiodicity
is discussed. Both energetic and entropic mechanisms may stabilize the
quasicrystalline phase. For systems where entropy plays the dominant
role, random tiling models are the appropriate description. These are
discrete statistical models, but without an underlying lattice. Severa
l, though very few, quasicrystalline random tilings have been solved e
xactly, in the sense that the free energy has been calculated analytic
ally in the thermodynamic limit. The models have besides a quasicrysta
lline phase also incommensurate phases of which the rotation symmetry
is that of an ordinary crystal. The quasicrystalline phase maximizes t
he entropy. (C) 1998 Elsevier Science B.V. All rights reserved.