A recently developed method of synthesis of T-extended porphyrins made it possible to prepare a series of tetrabenzoporphyrins (TBP) with different numbers of meso-aryl substituents. The photophysical parameters of free-bases and Pd complexes of meso-unsubstituted TBP's, 5,15-diaryl-TBP's (Ar2TBP's) and 5,10,15,20tetraaryl-TBP's (Ar4TBP's) were mea ' sured. For comparison, similarly meso-arylsubstituted porphyrins fused with nonaromatic cyclohexeno-rings, i.e. Ar,-tetracyclohexenoporphyrins (Ar,TCHP's, n = 0, 2, 4), were also synthesized and studied. Structural information was obtained by ab initio (DFT) calculations and X-ray crystallography. It was found that: 1) Free-base Ar4TBP's are strongly distorted out-of-plane (saddled), possess broadened, red-shifted spectra, short excited-state lifetimes and low fluorescence quantum yields (rfl = 2-3 ns, Ofl = 0.02-0.03). These features are characteristic of other nonplanar free-base porphyrins, including Ar4TCHP's. 2) Ar2TBP free-bases possess completely planar geometries, although with significant in-plane deformations. These deformations have practically no effect on the singlet excited-state properties of Ar2TBP's as compared to planar meso-unsubstituted TBP's. Both types of porphyrins retain strong fluorescence (Tfl = 10-12 ns, Ofl = 0.3-0.4), and their radiative rate constants (k,) are 3-4 times higher than those of planar H2TCHP's. 3) Nonplanar deformations dramatically enhance nonradiative decay of triplet states of regular Pd porphyrins. For example, planar PdTCHP phosphoresces with high quantum yield (95,ho, = 0.45, T,h, = 1118 us), while saddled PdPh4TCHP is practically nonemissive. In contrast, both ruffled and saddled PdAr,,TBP's retain strong phosphorescence at ambient temperatures (PdPh2TBP: 'Iph s = 496 ps, O,h., = 0. 15; PdPh4TBP: Tphos = 258,us, Ophos = 0.08). It appears that.7r-extension is capable of counterbalancing deleterious effects of nonplanar deformations on triplet emissivity of Pd porphyrins.