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Modern Polymer Spect..

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1700<br />

- CIO<br />

--- ca<br />

c 22<br />

_- c 12<br />

l l l l l l l l l<br />

Figure 3-5. Effect of the long-range interactions (s in equation 3.45) on the dispersion curves of the<br />

frequency branch v3 (associated with the in-phase skeletal stretching) of trms polyacetylene calculated<br />

for the unsimplified and realistic equilibrium geometry. The force field has been derived by ‘LI~J<br />

initio’ calculations on polyene oligoinei-s with n = 2,4,5,6, and 11 double bonds [%I. Attention<br />

should be paid to the fact that the ‘softening’ of the ~ ( = 90) mode iiiodulated by the distance of<br />

iriteraction generates a ‘dispersion’ with chain length of a very strong and very characteristic<br />

Ranian line ([41, 421).<br />

These observations are essential when the dynamics of disordered chains will be<br />

discussed later in this chapter.<br />

3.6 From Dynamics to Vibrational <strong>Spect</strong>ra of<br />

One-Dimensional Lattices<br />

The experiments which provide direct information on the vibrations of one- and<br />

tridimensional lattices are infrared absorption (reflection) spectra, Ranian scattering<br />

and neutron scattering. For a general discussion on the theoretical principles and<br />

experimental methods the reader is referred to the abundant literature on these

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