The incommensurate Frenkel-Kontorova model in its pinned phase is shown to
be equivalent to a system with correlated disorder. This correlated disorde
r appears as dimer-type "defects" on appropriately decimated lattices descr
ibing the phonon modes of the system. As a consequence of the special reson
ance condition where the reflected waves from two sites Of the dimer underg
o destructive interference, the decimated lattices exhibit Bloch-type phono
n modes for energies that can be tuned by varying the nonlinearity paramete
r of the system. In a generalized two-parameter model, where the strength a
nd the smoothness of the potential can be controlled independently, our stu
dy provides strong evidence of localization in a discrete quasiperiodic pot
ential with an infinite number of steps. This localization boundary interwi
nes with the parameter region exhibiting the Bloch-type states. [S0163-1829
(99)12113-1].