Excited states in a conjugated polymer are associated with excitation, relaxation, diffusion and decay processes, and their dynamical properties can be used to fabricate polymeric optoelectronic devices with higher efficiency. Although the timescale of excitonic radiative decay has been narrowed less than a nanosecond, the nonadiabatic mechanism presented in this article is able to provide a detailed depiction of the fluorescence dynamics with respect to singlet exciton decay and the evolution of the dipole moment. Simultaneously, it is found that the lifetime of the singlet exciton ranges from around 500 picoseconds to one nanosecond, which is in line with recent experimental observations on polymers such as benzothiadiazole and thiophene.Over several decades, since the growing demand for innovative functional devices in light of the global energy crisis, organic semiconducting materials have been favorably utilized to fabricate organic light emitting diodes (OLEDs), 1-5 organic solar cells (OSCs), 6-11 organic field effect transistors (OFETs), 12-14 and other promising devices. Given that the fabrication of these devices is based on excited states, researchers have to overcome the major challenge as to how to precisely describe and utilize the dynamical processes of excited states in organic semiconductors, including the processes of excitation, relaxation, formation, decay and interactions among different excited-state species. [15][16][17][18][19][20] With respect to dynamical processes of the singlet exciton, experimental research has relied on ultrafast spectroscopy to clarify the optoelectronic properties of conjugated polymer materials, such as poly(p-phenylenevinylene) (PPV) and its derivatives, 21-24 poly(thienylenevinylene) (PTV), 25 poly(dioctylfluorene) and its derivatives, 26,27 and poly (3-hexylthiophene)(P3HT) and its derivatives, 28,29 Especially, based on ultrafast pump-probe transient absorption (TA) spectroscopy in P3HT/PCBM([6,6]-phenyl-C61-butyric acid methyl ester) blends, the exciton decay timescale is shown to be around 0.9 ns. 30 For exciton relaxation in pristine PCDTBT, the lifetime of the exciton even can be broadened, ranging from 500 fs to a nanosecond. 31 Also, both in solution and solid film of P3HT-OH, the singlet exciton decay time is hundreds of picoseconds. 32,33 Recent temperature-independent absorption experiments have demonstrated that the lifetime of an exciton is just a reflection of the intrinsic physical properties of low-dimensional excitons rather than extrinsic disturbances, such as photoluminescence measurements. 34 Thus, in this article, we are presented with the task of how to accurately analyze the exciton's radiative decay in a quasi-one-dimensional conjugated polymer.Thus, after an exciton is formed in a polymer conductor, the description of its decay becomes an important step to understand the whole dynamical process of excited states. Therefore, we move our concentration to one-dimensional semiconductors, such as hole-doped single-walled carbon nanotubes, whe...