Soluble alkyl (II, 8a,b), fluoroalkyl (4a), and fluoroalkoxy (4b,c, 8c) 1,(4)- or 2,(3)-substituted
phthalocyaninato- and linear 2,(3)- and angular 1,(2)-annulated naphthalocyaninatotitanium(IV) oxides 10,
12, and 14 were synthesized and characterized with regard to their spectroscopic, photophysical, and
photochemical properties. While alkyl- and fluoroalkoxy-substituted compounds are highly soluble in nonpolar
solvents, e.g., hexane, fluoroalkyl-substituted compounds are better soluble in polar aprotic solvents such as
acetone. The stability against photooxidation in solution is enhanced on going from alkylated phthalocyanines
1,(4)-(C5H11)8PcTiO (8a), 1,(4)-(C6H13)8PcTiO (8b), and 2,(3)-(C4H9)8PcTiO (II) to fluorinated phthalocyanines
2,(3)-(CF3)4PcTiO (4a), 2,(3)-(CF3CH2O)4PcTiO (4b), and 2,(3)-(CF3CH2O)8PcTiO (4c), from phthalocyanines
to naphthalocyanines (tert-butyl)4-2,(3)-NcTiO (10), 1,(2)-NcTiO (12), and (tert-butyl)4-1,(2)-NcTiO (14), and
on going from 2,(3)-substituted 4a−c to 1,(4)-substituted phthalocyanines 8a−c. Thin films of these compounds,
prepared by either vacuum deposition or spin casting, are classified into three types according to increasing
intermolecular π−π interactions. Type α films, characterized by absence of exciton splitting, are formed
from 1,(4)-substituted phthalocyanines 8a−c. These films show low dark conductivities and photoconductivities
and are considerably sensitive to photooxidation. Type β films, characterized by weak exciton splitting, are
formed from fluorinated phthalocyanines 4a−c as well as from rapidly deposited 2,(3)-substituted phthalocyanines II and the unsubstituted PcTiO (I). These films show enhanced photoconductivity and are generally
more stable against photooxidation than type α films. Type γ films, formed by slow deposition of II, 10 and
unsubstituted phthalocyanine I, are classified by a largely red-shifted B-band absorbing in the near-IR. These
films are highly photosensitive as well as stabilized against photooxidation. Steady-state photoconductivities
and dark conductivities in thin films are strongly dependent on oxygen partial pressure. Alkylated PcTiO's
such as 8a, 8b, and II are found to be p-type conductors (positive oxygen influence on conductivities) like
unsubstituted PcTiO (I), whereas angularly annulated naphthalocyanines such as 12 and 14 as well as fluorinated
PcTiO's 4a−c are n-type conductors (negative oxygen influence on conductivity). These findings are
rationalized by comparison with experimental and theoretical literature data.