potentials in terms of both performance and cost efficiency. Identifying new lowcost materials for high performance LEDs that can be facilely processed is of great interest scientifically and practically.Recently, metal halide perovskites and perovskite-related materials have emerged as new generation light emitting materials with remarkable and highly tunable optical properties. [8] To date, efficient near-infrared, red, green and blue perovskite LEDs have been demonstrated with external quantum efficiencies (EQEs) of up to 22.2%, [9] 24.4%, [10] 28.1%, [11] and 13.8%, [12] respectively. While perovskite LEDs have shown great potentials, lead containing devices represent a major environmental and health concern that could limit their wide commercialization. Moreover, most halide perovskites and perovskite-related structures are metastable under normal atmospheric conditions, which is another obstacle to achieve devices with long lifetimes. [1] In searching for efficient lead-free perovskite-related light emitting materials with high stability, great progress has been made on zero-dimensional (0D) organic metal halide hybrids (OMHHs), which contain light emitting metal halide polyhedra fully isolated and surrounded by bulky organic cations. [13] Due to the complete site isolation, 0D OMHHs possess a perfect "host-dopant" structure, with light emitting metal halide species periodically embedded in a large bandgap organic host matrix. [14] While high PLQEs of up to near-unity have been routinely achieved in numerous 0D OMHHs, their applications in electrically driven LEDs have been under explored with very few reports to date. [15] The poor conductivity and wide bandgap of organic cations are the major factors responsible for the inferior charge transport and energy level alignment in these low performance LEDs based on 0D OMHHs. [14] Here, we report a simple molecular engineering approach to addressing the issues of low conductivity and poor energy alignment in electrically driven LEDs based on 0D OMHHs. By introducing a simple organic charge transporting unit (phenylcarbazole) to previously studied triphenyl(9-phenyl-9H-carbazol-3-yl) phosphonium (TPP + ) cation, we have developed a semiconducting organic cation, triphenyl(9-phenyl-9H-carbazol-3-yl) phosphonium (TPPcarz + ). [16] A 0D OMHH TPPcarzSbBr 4 was then synthesized for the first time, in which light emitting