T. Kanaya et al., Orientational effects on low-energy modes in amorphous poly(ethylene terephthalate) fiber, J CHEM PHYS, 109(23), 1998, pp. 10456-10463
Inelastic and quasielastic neutron-scattering measurements have been perfor
med on an amorphous poly(ethylene terephthalate) (PET) fiber in parallel an
d perpendicular scattering geometries., i.e., when the fiber axis f is para
llel and perpendicular to the scattering vector Q, respectively. The so-cal
led boson peak is observed at around -1.4 meV in neutron energy transfer at
low temperatures below about 150 K in both the geometries; as temperature
increases, the fast process of picosecond order appears at a certain temper
ature below the glass-transition temperature T-g (= 348 K). Although no dra
stic differences in the dynamics can be observed, a closer look at the spec
tra revealed some interesting features of the low-energy modes. From the me
an-square displacements evaluated with two different energy resolutions, it
was found that the fast process appears only in the direction perpendicula
r to the polymer chain (not the fiber axis f) in the energy region between
-1 and -0.2 meV. In the inelastic scattering spectra, we found that the bos
on peak is stronger in intensity for the parallel direction while the inten
sity of the fast process is larger for the perpendicular one. The quantitat
ive analysis based on the recent vibration-relaxation model revealed that t
he fast process can mainly be explained by the softening of the vibrational
modes; the softening occurs at lower temperatures in the perpendicular geo
metry than in the parallel one. On the other hand, the conventional single-
lorentzian fit to the fast process, in which the fast process is assumed to
be a relaxational process and described by a Lorentzian, showed that the o
nset temperature of the fast process is lower in the perpendicular geometry
than in the parallel one. These have been tentatively attributed to weaker
force constants, for motions perpendicular to a polymer chain, such as tor
sional and librational motions, than those along the chain. (C) 1998 Americ
an Institute of Physics. [S0021-9606(98)50347-9].