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-1. This is merely the consequence of a negligible dynamical coupling between bending and stretching vibrations. Moreover, the choice of a linear geometry for oligomers makes it possible to assume the same symmetry for short chains and for the infinite 1D crystal, thus making the comparison easier.
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-1. This is merely the consequence of a negligible dynamical coupling between bending and stretching vibrations. Moreover, the choice of a linear geometry for oligomers makes it possible to assume the same symmetry for short chains and for the infinite 1D crystal, thus making the comparison easier.
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n refers to the interaction between nonequivalent bonds at distance n. The symbols appearing in eq 2 can be collected in a usual matrix representation of the force constant matrix F of the infinite chain (see Supporting Information).
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n refers to the interaction between nonequivalent bonds at distance n. The symbols appearing in eq 2 can be collected in a usual matrix representation of the force constant matrix F of the infinite chain (see Supporting Information).
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36748998613
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The plot of Fig. 3 has been obtained by using force constants transferred from the scaled force field obtained from a PBE1PBE/cc-pVTZ calculation (see discussion in section III), but the same qualitative results are obtained using unsealed DFT force fields of the same molecule.
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The plot of Fig. 3 has been obtained by using force constants transferred from the scaled force field obtained from a PBE1PBE/cc-pVTZ calculation (see discussion in section III), but the same qualitative results are obtained using unsealed DFT force fields of the same molecule.
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The choice of the functional PBE1PBE and of the basis set cc-pVTZ is motivated by the fact that it seems to be the method which can better reproduce the relative intensities of the α and β lines (see Figure 1).
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The choice of the functional PBE1PBE and of the basis set cc-pVTZ is motivated by the fact that it seems to be the method which can better reproduce the relative intensities of the α and β lines (see Figure 1).
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