D. Schlettwein et al., Substrate-induced order and multilayer epitaxial growth of substituted phthalocyanine thin films, LANGMUIR, 16(6), 2000, pp. 2872-2881
Thin films of hexadecafluorophthalocyaninatooxovanadium (F16PcVO) are vapor
-deposited under organic molecular beam epitaxy (OMBE) conditions on the (1
00) surfaces of NaCl, KCl, and KBr and on quartz glass. Beginning at submon
olayer coverages and extending to a film thickness of several tens of nanom
eters the film structure is determined in situ by reflection high energy el
ectron diffraction (RHEED). Following deposition the film morphology is cha
racterized by tapping mode atomic force microscopy (AFM) and chromophore co
upling of the molecules within the films is studied by optical absorption s
pectroscopy. Highly ordered growth of crystalline domains of F16PcVO with d
imensions in the micrometer range leading to films of quite uniform thickne
ss is observed. On KBr a commensurate root 10 x root 10, R = 18.4 degrees s
quare lattice is seen in RHEED of the first monolayers with the molecules p
arallel to the substrate surface which is also preserved at higher film thi
ckness. On KCI a surface lattice of the same size is formed which is, howev
er, understood as a result of point-on-line coincidence. Diffraction of tra
nsmitted electrons yield a constant three-dimensional crystal structure of
the films on kBr and KCl with a tetragonal unit cell of a = b = 1.47 nn and
c = 0.62 nm. On NaCl with its smaller lattice constant no ordered relative
orientation is possible and hence an increased part of the film appears am
orphous. On quartz glass on the other hand, ordered films are formed with t
he molecular plane predominantly oriented cofacially parallel to each other
and vertical to the surface. Calculations of molecular mechanics as well a
s of periodic surface potentials are performed to support the proposed stru
ctures and to discuss the crystallization in thin films of phthalocyanines
and related materials. Implications of the present results for the electric
al properties to be expected from such layers and their potential use in mo
lecular semiconductor thin films are discussed.