photovoltaic cells, [4,5] sensors, [6] and fieldeffect transistors [7] by both academic and industrial research teams. In the past decades, great progress has been made in organic and polymeric semiconductor materials, which brings up the possibility for the ultimate realization of organic diode laser-a conundrum in organic semiconductor field. [8] Early in 1996, solidstate organic lasing has been successfully demonstrated by Hide et al. [9] from an optically pumped thin-film waveguide of MEH-PPV/polystyrene film, while Tessler et al. [10] made the first vertical microcavity laser based on conjugated polymers as gain materials. Subsequently, optically pumped lasers has been demonstrated in a broad range of conjugated polymers, oligomers, and evaporated small molecular films. [11][12][13][14] Most recently, low threshold lasing under quasi continuous-wave photo excitation was reported by Adachi and coworkers [15] Despite success in optically pumped lasing, the electrically pumped "injection laser" remains as a significant challenge.From the aspect of optical loss, an important criterion for high-performance laser gain medium is the optical transparency. In this sense, ideal laser material candidates should be single crystals or fully amorphous materials (such as glass). As for further realization of electrically pumped lasing, the gain medium also requires high carrier mobility to achieve considerable current density injection; meanwhile, it should have relatively simple relaxation behavior of excited states to exclude additional optical losses such as polaron [16] and triplet [17] formations. Based on these, low threshold gain materials with minimum optical loss are highly demanded.Herein, we develop a benzothiadiazole-cored multifluorene derivative, named OCBzC, with similar molecular backbone to F8BT. (Figure 1a) High quality lasing is demonstrated on its microring resonator. The excellent photoluminescence properties with an amorphous morphology [18] and a low waveguide loss in films have inspired us to focus on the origin of its low intrinsic optical loss from the transient dynamics of excited state.A simple microring resonator is fabricated by drop-casting the 20 mg mL −1 OCBzC solution (chlorobenzene solvent) onto a silica optical microfibre with a diameter of 10 µm. Notably, both the fluorescence microscopic image and scanning electron Meeting the challenges of realizing organic electrically pumped laser, low threshold gain materials with minimum optical loss are highly demanded, especially those with insignificant nonradiative processes during lasing. Herein, the low optical loss amplified spontaneous emission (ASE) and high Q-factor (2,700) lasing are discovered in a solution-processed benzothiadiazole-cored multifluorene derivative. The excellent lasing properties of this molecule inspire to focus on the origin of its intrinsic optical loss. The ultrafast time-resolved spectroscopy studies reveal that the low intrinsic optical loss originates from a relatively "simple" excited state interaction includin...