Hy. Wang et al., STRUCTURAL INVESTIGATION OF GAS-SENSING LANGMUIR-BLODGETT-FILMS OF PHTHALOCYANINE ((C6H13)(3)SIOSIPCOGEPCOH), Thin solid films, 273(1-2), 1996, pp. 90-96
The crystal structure of the phthalocyanine ((C6H13)(3)SiOSiPcOGePcOH)
(abbreviated as Si-Ge Pc dimer) Langmuir-Blodgett (LB) film was inves
tigated using X-ray and electron diffraction to provide a structural b
asis for the observed conductivity change upon gas doping. The structu
re refinement was done using the linked-atom least-squares method. The
structure determined for the Si-Ge Pc dimer is believed to result fro
m the film deposition mechanism and is as follows: crystal system, mon
oclinic; space group, Pn; a = b = 14.28 Angstrom, c = 23.40 Angstrom,
alpha = beta = 90 degrees, V = 4772 Angstrom(3), Z = 2, and the calcul
ated density is 1.015 g cm(-3). The staggering angle between the two P
c rings is 5.5 degrees and the final R value is 9.23%. It is the trihe
xyl tail group in the molecule that breaks the symmetry of the system
and gives rise to the low film density. The phthalocyanine LB films ha
ve been used successfully as gas sensors and the gas-sensing mechanism
has been modeled as gas adsorption on the film surface and then diffu
sion through the film. It is the low density and open structure of the
film that facilitate the gas diffusion through the film and the charg
e transfer interactions between the gas molecules and the phthalocyani
ne rings, which give rise to the high sensitivity and fast response of
the gas sensor.