How, in principle, could one solve the atomic structure of a quasicrystal,
modeled as a random tiling decorated by atoms, and what techniques are avai
lable to do it? One path is to solve the phase problem first, obtaining the
density in a higher dimensional space which yields the averaged scattering
density in 3-dimensional space by the usual construction of an incommensur
ate cut. A novel direct method for this is summarized and applied to an i(A
LPdMn) data set. This averaged density falls short of a hue structure deter
mination (which would reveal the typical unaveraged atomic patterns.) We di
scuss the problematic validity of inferring an ideal structure by simply fa
ctoring out a "perp-space" Debye-Waller factor, and we test this using simu
lations of rhombohedral tilings. A second, "unified" path is to relate the
measured and modeled intensities directly, by adjusting parameters in a sim
ulation to optimize the fit. This approach is well suited for unifying stru
ctural information from diffraction and from minimizing total energies deri
ved ultimately from ab-initio calculations. Finally, we discuss the special
pitfalls of fitting random-tiling decagonal phases.