“…According to the charge density distribution of S 1 states, the large size of C 3 N QDs with a diameter of 1.66−1.82 nm (named C 36 N 12 , α-C 36 N 12 and C 30 N 10 ) shows significant electron−hole separation in real space involving the high excited state dipole moment (D Sd 1 = 3.48−4.95 D), which is not conducive to the occurrence of radiation transitions. In the case of smaller QDs (C 12 N 4 , C 18 N 6 , α-C 18 N 6 , C 24 N 8 , and α-C 24 N 8 ), the electron−hole pairs are not significantly separated and show uneven distribution, which results in asymmetric variations of the electron structure in QDs, and electron−hole pairs break the orbital transition symmetry barrier, ultimately leading to radiative recombination, which is well consistent with experimental report that the smaller C 3 N QDs have a large quantum yield (QY > 80%) 27. In experiments, carbonbased QDs are usually synthesized by the solvothermal method; we further explored the solvent effects on fluorescence performances of C 3 N QDs.…”