The atomic structure of quasicrystals(1)-solids with long-range order,
but non-periodic atomic lattice structure-is often described as the t
hree-dimensional generalization of the planar two-tile Penrose pattern
(2). Recently, an alternative model has been proposed(3-5) that descri
bes such structures in terms of a single repeating unit(3-5)-the three
-dimensional generalization of a pattern composed of identical decagon
s. This model is similar in concept to the unit-cell description of pe
riodic crystals, with the decagon playing the role of a 'quasi-unit ce
ll'. But, unlike the unit cells in periodic crystals, these quasi-unit
cells,overlap their neighbours, in the sense that they share atoms. N
evertheless, the basic concept of unit cells in both periodic crystals
and quasicrystals is essentially the same: solving the entire atomic
structure of the solid reduces to determining the distribution of atom
s in the unit cell. Here we report experimental evidence for the quasi
-unit-cell model by solving the structure of the decagonal quasicrysta
l Al72Ni20Co8. The resulting structure is consistent with images obtai
ned by electron and X-ray diffraction, and agrees with the measured st
oichiometry, density and symmetry of the compound. The quasi-unit-cell
model provides a significantly better fit to these results than all p
revious alternative models, including Penrose tiling.