Fluorene is a blue luminous moiety attracting wide attention due to its all kinds of high technology applications, and the rigid biphenyl planar structure of fluorene makes it prone to crystalize and form intermolecular aggregation, which means that emitting colors and carrier mobilities of fluorene-based fluorescence emitters are highly adjustable by the modification of 9,9-position of fluorene with different pendant moieties. In this regard, fluorene (F) is used as a model blue emitter, and different pendant groups of n-butyl, p-hexyloxy phenyl and 2,4,6-triphenyl-1,3,5-triazine are introduced into the 9-position of fluorene to produce four topology-varied organic light-emitting emitters, namely 9,9-dibutyl-fluorene (DBF), 9,9-bis-(4-butoxy-phenyl)-fluorene (BOPF), 2-{4-[9-(4-hexyloxy-phenyl)-fluoren-9-yl]-phenyl}-4,6-diphenyl- (Chan et al., 2017; Wex and Kaafarani, 2017; Liang et al., 2019) [1,3,5]triazine (FTRZ) and 2,4,6-tris-{4-[9-(4-hexyloxy-phenyl) -fluoren-9-yl]-phenyl}- (Chan et al., 2017; Wex and Kaafarani, 2017; Liang et al., 2019) [1,3,5]triazine (pTFTRZ). The general differences in thermal stability, photoluminescence quantum efficiency, emission wavelength, electrochemical energy levels, crystal structure, carrier mobility and film morphology of the emitters are experimentally and theoretically studied to correlate their structures with optoelectronic properties. FTRZ and pTFTRZ solid powder show higher melting points of 186 °C and 122 °C. The highest occupied molecular orbit energy levels are −5.95 eV for F , −6.02 eV for DBF , −6.11 eV for BOPF and −6.23 eV for FTRZ , and the corresponding lowest unoccupied molecular orbits energy levels are −2.03 eV for F , −2.19 eV for DBF , −2.25 eV for BOPF and −2.55 eV for FTRZ. When compared with the other three emitters, due to the enhanced intramolecular charge transfer caused by the electron-deficient 2,4,6-triphenyl-1,3,5-triazine group, FTRZ showed significant redshifts of 75 nm in their emission spectrum of solution, and the photoluminescence quantum efficiencies of FTRZ and pTFTRZ solid powder were also decreased to less than 1%. The single crystal of F is an orthorhombic system while those of DBF , BOPF and FTRZ are all monoclinic system. The electron and hole mobilities of the thin solid films were decreased in the order of FTRZ , BOPF and pTFTRZ , and thin solid film of FTRZ showed the highest electron mobility of 10−4cm2/V • s at an electric field of 4 × 104 V/cm. The RMS values corresponding to root-mean-square averages of the height deviations of film measured by atomic force microscopy are 4.32 nm for BOPF , 1.11 nm for FTRZ , 11.8 nm for pTFTRZ. The FTRZ films exhibited smaller RMS and smooth surface morphology beneficial for the carrier mobility relative to those of BOPF and pTFTRZ. The pendant groups of n-butyl, p-hexyloxy phenyl and 2,4,6-triphenyl-1,3,5-triazine in the 9-position of fluorene adjust the general optoelectronic properties of the obtained emitters in a wide range. • FTRZ and pTFTRZ solid powders show higher melting points of 186 °C and 122 °C; • The carrier mobilities of the FTRZ , BOPF and pTFTRZ thin solid films decreased in turn; • The PLQYs of FTRZ and pTFTRZ solid powders decreased to less than 1%; • The single crystal of F is an orthorhombic system while those of DBF , BOPF and FTRZ are all monoclinic system; • The FTRZ films exhibited smaller RMS beneficial for the improved carrier mobilities. [ABSTRACT FROM AUTHOR]