Abstract:A series of pyrene derivatives having 4-(N,N-dimethylamino)phenylethynyl groups as the substituent (1-5) have been synthesized and their two-photon absorption properties were investigated. Comparison of two-photon cross section (delta(max)) with related compounds reveals that pyrene is as efficient a pi-center as anthracene in two-photon materials. Moreover, the two-photon cross section (delta(max)) increased with the number of substituents reaching at the maximum value of 1150 GM for the tetra-substituted der… Show more
“…The dihedral angle between the plane of the triphenylene ring and the plane of the phenyl ring is 96° for 1g . These observations are comparable with the geometry of the corresponding pyrene derivatives reported earlier [31–32]. The HOMO and LUMO surfaces are shown in Fig.…”
SummarySeveral 2-(phenylethynyl)triphenylene derivatives bearing electron donor and acceptor substituents on the phenyl rings have been synthesized. The absorption and fluorescence emission properties of these molecules have been studied in solvents of different polarity. For a given derivative, solvent polarity had minimal effect on the absorption maxima. However, for a given solvent the absorption maxima red shifted with increasing conjugation of the substituent. The fluorescence emission of these derivatives was very sensitive to solvent polarity. In the presence of strongly electron withdrawing (–CN) and strongly electron donating (–NMe2) substituents large Stokes shifts (up to 130 nm, 7828 cm−1) were observed in DMSO. In the presence of carbonyl substituents (–COMe and –COPh), the largest Stokes shift (140 nm, 8163 cm−1) was observed in ethanol. Linear correlation was observed for the Stokes shifts in a Lippert–Mataga plot. Linear correlation of Stokes shift was also observed with E
T(30) scale for protic and aprotic solvents but with different slopes. These results indicate that the fluorescence emission arises from excited state intramolecular charge transfer in these molecules where the triphenylene chromophore acts either as a donor or as an acceptor depending upon the nature of the substituent on the phenyl ring. HOMO–LUMO energy gaps have been estimated from the electrochemical and spectral data for these derivatives. The HOMO and LUMO surfaces were obtained from DFT calculations.
“…The dihedral angle between the plane of the triphenylene ring and the plane of the phenyl ring is 96° for 1g . These observations are comparable with the geometry of the corresponding pyrene derivatives reported earlier [31–32]. The HOMO and LUMO surfaces are shown in Fig.…”
SummarySeveral 2-(phenylethynyl)triphenylene derivatives bearing electron donor and acceptor substituents on the phenyl rings have been synthesized. The absorption and fluorescence emission properties of these molecules have been studied in solvents of different polarity. For a given derivative, solvent polarity had minimal effect on the absorption maxima. However, for a given solvent the absorption maxima red shifted with increasing conjugation of the substituent. The fluorescence emission of these derivatives was very sensitive to solvent polarity. In the presence of strongly electron withdrawing (–CN) and strongly electron donating (–NMe2) substituents large Stokes shifts (up to 130 nm, 7828 cm−1) were observed in DMSO. In the presence of carbonyl substituents (–COMe and –COPh), the largest Stokes shift (140 nm, 8163 cm−1) was observed in ethanol. Linear correlation was observed for the Stokes shifts in a Lippert–Mataga plot. Linear correlation of Stokes shift was also observed with E
T(30) scale for protic and aprotic solvents but with different slopes. These results indicate that the fluorescence emission arises from excited state intramolecular charge transfer in these molecules where the triphenylene chromophore acts either as a donor or as an acceptor depending upon the nature of the substituent on the phenyl ring. HOMO–LUMO energy gaps have been estimated from the electrochemical and spectral data for these derivatives. The HOMO and LUMO surfaces were obtained from DFT calculations.
“…For example, the emission maxima of the pyrenyl-substituted pyrenes 6, 7a/7b, and 8, consecutively shifted to longer wavelengths at 432, 451 and 465 nm respectively ( Figure 4a), in a manner similar to their absorption maxima. These results were also observed in some carbazole-based dendrimers [46] and several phenylethynyl-substituted pyrene derivatives [47,48]. Similar findings were observed in the tetrakisfluorenyl-substituted pyrene 10 ( max = 456 nm, red-shifted ca.…”
Three types of stable pyrene-based highly fluorescence (blue) compounds, 1-, 1,6-bis, 1,8-bis and 1,3,6,8-tetrakis(7-tert-butylpyrenyl)pyrenes and 1, 3,6,8-tetrakis[9,9-bis
“…Pyrene and its derivatives have been studied intensively as organic chromophores [5,6], sensors [7,8], light emitting materials in OLEDs [9][10][11][12], organic field effect transistors (OFETs) [12,13] and organic photovoltaic devices (OPVs) [12]. Synthetic pyrene-appended systems are used as sensors for ATP [14], heparin [15], nucleotides [16,17], transition metal ions [18] and as probes to study protein conformation, conformational changes, protein folding and unfolding, protein-protein, protein-lipid, and protein-membrane interactions [19].…”
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