“…adducts with both - and -donors show one main peak in their FT-Raman spectra in the range 190–140 cm −1 [16, 59, 60, 62–67, 81] at a lower frequency with respect to solid [216 cm −1 , d (I−Br) = 2.521(4) Å] [98], and it is assignable to a stretching vibration of the E−I−Br three-body system having a major contribution from the ν (I−Br) vibration [63]. adducts (only four out of seven are both structurally and vibrationally characterized) [60, 67, 68]
generally show in their FT-Raman spectra two main peaks: one in
the range 240–180 cm −1 presumably due to the
antisymmetric ( ν
3 ) stretching vibration of the
E−I−Cl three body-system
( = , ), and the other at about
130 cm −1 due to the symmetric ( ν
1 ) stretching vibration (solid is characterized by a single peak at 283 cm −1 in its FT-Raman spectrum with a
d (I−Cl) = 2.446(6) Å) [99]. Interestingly, by considering the Δ d (I−Y) parameter
( = , , ), a linear correlation appears also to exist between Δ d (I−Br) and ν (I−Br) for adducts, and between Δ d (I−Cl) and the ν (E−I−Cl) stretching mode corresponding to the ν
antisym in symmetric three-body systems, for adducts (Figure 8).…”