MOLECULAR-ORIENTATION AND STRUCTURE IN EVAPORATED-FILMS OF 2-DODECYL-7,7,8,8-TETRACYANOQUINODIMETHANE, 2-PENTADECYL-7,7,8,8-TETRACYANOQUINODIMETHANE, AND 2-OCTADECYL-7,7,8,8-TETRACYANOQUINODIMETHANE STUDIED BYINFRARED AND RAMAN-SPECTROSCOPY
A. Nakagoshi et al., MOLECULAR-ORIENTATION AND STRUCTURE IN EVAPORATED-FILMS OF 2-DODECYL-7,7,8,8-TETRACYANOQUINODIMETHANE, 2-PENTADECYL-7,7,8,8-TETRACYANOQUINODIMETHANE, AND 2-OCTADECYL-7,7,8,8-TETRACYANOQUINODIMETHANE STUDIED BYINFRARED AND RAMAN-SPECTROSCOPY, Langmuir, 10(3), 1994, pp. 779-783
Infrared and Raman spectra have been measured for evaporated films of
2-dodecyl-7,7,8,8-tetracy-anoquinodimethane (dodecyl-TCNQ), 2-pentadec
yl-7,7,8,8-tetracyanoquinodimethane (pentadecyl-TCNQ), and 2-octadecyl
-7,7,8,8-tetracyanoquinodimethane (octadecyl-TCNQ) deposited onto Au-
or Ag-evaporated glass slides or CaF2 plates, and the obtained spectra
have been compared with those of their Langmuir-Blodgett (LB) films p
reviously. The relative intensities of infrared bands in the reflectio
n-absorption (RA) spectrum indicate that the molecular orientation in
the evaporated film of dodecyl-TCNQ on the Au- or Ag-evaporated glass
slide is very close to that in its LB film; the hydrocarbon chain is t
ilted largely with its molecular plane nearly parallel to the surface
and the TCNQ plane is nearly perpendicular to the surface in both film
s. The molecular orientation in the evaporated film of pentadecyl-TCNQ
on the Au-or Ag-evaporated glass slide is also similar to that in its
LB film. However, the molecular orientation in the evaporated film of
octadecyl-TCNQ on the Au- or Ag-evaporated glass slide is markedly di
fferent from that in its LB film; the alkyl chain of octadecyl-TCNQ is
tilted largely with its molecular plane nearly perpendicular to the s
urface and the TCNQ plane is inclined largely in the evaporated film.
The molecular orientation in the evaporated films of octadecyl-TCNQ sh
ows clear substrate dependency; the alkyl chain in the films on the Ca
F2 Plate is not so largely tilted as that on the Au- or Ag-evaporated
glass slide. The infrared and Raman frequencies of the bands arising f
rom the TCNQ chromophore do not change between the spectra of the evap
orated films and those of the solid states for the three alkyl-TCNQ co
mpounds. These observations lead us to conclude that the interaction b
etween the TCNQ part and Au or Ag surface is very weak.