Far-infrared transmittance measurements are performed on a series of i
sotopically labeled samples of the quasi-one-dimensional solids [Pt(en
)2][Pt(en2X2][ClO4]4, (en) = ethylenediamine and X = Cl, Br, or 1. Pro
nounced shifts upon deuteration of the (en) ligands reveal that severa
l absorption features previously attributed to localized vibrational m
odes of chain defects are in fact (en) ligand modes. Recognition of th
ese ligand modes resolves the previous ambiguity over the assignment o
f the infrared-active chain phonons, permitting the unambiguous assign
ment of the 238.7-cm-1 feature in the bromide material to the asymmetr
ic stretch (v2) chain phonon, and strongly suggesting the 184.2-cm-1 f
eature in the iodide is the V2 phonon of that material. A high-resolut
ion examination of the chloride, prepared with both natural Cl isotopi
c abundance and with nearly pure Cl-35 , reveals a Cl isotopic fine st
ructure that allows conclusive identification of the 359.1-cm-1 featur
e as the V2 chain phonon. Lattice-dynamics calculations using a harmon
ic-linear-chain model with randomly distributed Cl isotopes yield good
agreement with experiment and reveal that isotopic disorder leads to
pronounced vibrational localization in PtCl, with the observed fine st
ructure arising from modes residing on a few distinct sequences of iso
topes occurring with high probability. The radical difference between
the infrared fine structure of PtCl and that previously reported for t
he Raman-active chain mode is found to result from differences in the
dispersion curves for the two phonon branches, and allows indirect det
ermination of these dispersion curves.