Hybridization of boron subphthalocyanine (BsubPc) and boron subnaphthalocyanine (BsubNc) has been modestly explored in the past, and was therefore carried out herein to access a subclass of these chromophores denoted as R a -F x Bsub(Pc 3−p -Nc p ) hybrids, where R a is the axial halide substituent (axial chloride, Cl-, or axial fluoride, F-), x = 8, and p = 1. These chromophores were targeted as new candidate materials for organic electronic applications due to their C s symmetry, in-plane dipole moment, and unique photophysical properties. Cl-/F-F 8 Bsub(Pc 2 -Nc 1 ) hybrids were compared to Cl-/F-F 8 BsubPc hybrids, which are analogous compounds with an identical number of peripheral fluorine atoms but lower degree of π-conjugation. Upon photoexcitation of dilute toluene solutions and doped thin films with polystyrene as a nonemissive host, F 8 Bsub(Pc 2 -Nc 1 ) hybrids exhibited distinctively broad absorption spectra and narrow emission profiles with red-shifted peak photoluminescence wavelengths in the 618−623 nm region compared to F 8 BsubPc hybrids (581−584 nm). Electroluminescence properties were probed in simple solution-cast organic light-emitting diodes (OLEDs) in which all four hybrids were diluted within an F8BT emissive polymer host. Upon electronic excitation, electroluminescence (EL) of C s -symmetric hybrids followed the same trends as photoluminescence (PL), with OLED devices displaying narrow EL in the orange region (588−592 nm) for F 8 BsubPc hybrids and in the near-red region for F 8 Bsub(Pc 2 -Nc 1 ) hybrids (627−632 nm). The photophysical processes important to OLEDs moderately improved with less π-conjugation in the periphery of the C s -symmetric hybrids [F 8 Bsub(Pc 2 -Nc 1 ) vs F 8 BsubPc; EQE Max : 0.099% vs 0.129%; luminance: 500 cd/m 2 vs 1000 cd/m 2 at maximum current density; relative PL quantum yields (QYs) ≈ 17−22% vs ≈ 35−44%]. Electrochemical data showed that C s symmetry introduces reversibility or quasi-reversibility in the oxidation regime at potentials >1 V, and peripheral fluorination enables reversibility in the reduction process. Overall, F 8 Bsub(Pc 2 -Nc 1 ) hybrids embody several unique physical characteristics into one: broad absorption spectra (full width at half-maximum height, FWHM sol abs = 53−55 nm, FWHM film abs = 71 nm), narrow near-red electroluminescence (FWHM OLED EL = 33 nm), and photoluminescence (FWHM sol PL = 25−26 nm, FWHM film PL = 32 nm) emission, small energy band gaps (1.95−1.96 eV), high extinction coefficients (ε ≈ (5.65−6.16) × 10 4 M −1 cm −1 ), and dual electrochemical versatility. These results provide new physical insights into the material properties of C s -symmetric macrocycles and advance the consideration of F 8 Bsub(Pc 2 -Nc 1 ) and F 8 BsubPc hybrids for optoelectronic applications.