Neil G. Pschirer, Mary E. Vaughn, Y. B. Dong, Hans-Conrad zur Loye and Uwe H. F. Bunz*
Department of Chemistry and, Biochemistry, The University of South Carolina, Columbia, South Carolina 29208, USA.. E-mail: bunz@psc.sc.edu
First published on UnassignedUnassigned6th January 2000
Synthesis of poly(p-phenyleneethynylene)s (PPEs) containing 1,5-diethynyl-3,7-di-tert-butylnaphthalene leads to novel phenylene-naphthylene-ethynylene copolymers which show strong blue luminescence in the solid state.
Herein we repot the synthesis and characterization of the unsaturated copolymers 3 which are efficient blue emitters in the solid state (Fig. 1). The polymers 3 are obtained by adding defined amounts of 3,7-di-tert-butyl-1,5-dipropynylnaphthalene 27 to 1,4-dipropynyl-2,5-dialkylbenzenes 1 (Scheme 1) in our alkyne metathesis protocol utilizing an instant catalyst formed of Mo(CO)6 and 4-chlorophenol.8† The catalyst and a varying ratio of monomers 1 and 2 were stirred in 1,2-dichlorobenzene at 140 °C for 11–25 h under a flow of N2. This protocol results in a series of high molecular weight copolymers 3. Longer polymerization times give rise to higher degrees of polymerization, as examined in the PPE system in detail.8
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Fig. 1 Solid-state emission (hand held fluorescence lamp, λmax = 366 nm) of PPE and PPE-napthalene copolymers 3: (a) didodecyl-PPE; (b) polymer 3a; (c) polymer 3c; (d) polymer 3d; (e) poly(3,7-di-tert-butylnaphtyleneethynylene). |
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Scheme 1 |
The UV–VIS spectra of 3a–d in dilute solution show a λmax of 388–395 nm, very similar to that of dialkyl-PPEs (388 nm). To our surprise, thin film absorption spectra of 3a–d are identical to those in solution, which is in stark contrast to the PPE case where a dramatic red-shift is observed. The unusual optical behavior prompted us to investigate fluorescence of 3a–d. In solution an intense blue emission is observed (3a, 425 nm; 3d, 419 nm), again similar to dialkyl-PPEs (425 nm). In the solid state, however, the situation is different, and in thin films of 3a–d we find emission maxima ranging from 446 (5∶1, 3a) to 422 nm (1∶2, 3d), (Fig. 2), thus allowing the manipulation of solid-state emission maximum from yellow–green to blue via the amount of added monomer 2. The less PPE character the copolymer 3 has, the further its emission is blue-shifted towards that observed in dilute solution. We conclude that in the copolymers 3 aggregation and supramolecular ordering are efficiently suppressed by the presence of the bulky tert-butylnaphthyl groups.9 This scenario must lead to a disordered solid state in 3. To test this hypothesis we performed powder diffraction on polymers 3 (Fig. 3). The polymers 3a–c display a broad diffraction peak of large intensity according to d = 4.2 Å. This diffraction peak can be attributed to the interchain distance of the polymers. A second, weak diffraction peak is observed at d = 8.8–11.7 Å, but is very weak in 3a–c. In the naphthalene-rich polymer 3d the small-angle diffraction at 11.7 Å is most prevalent. Molecular modeling indicates that this represents the distance between the two 3,7-tert-butyl groups on individual naphthalene units.10
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Fig. 2 Solid-state emission spectra of thin films of 3a–d and PPE. |
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Fig. 3 Diffraction data of polymers 3a–d. |
For device purposes, liquid crystalline behavior offers the entry to polarized emission. DSC and polarizing microscopy performed upon 3a–c shows that 3a,b are thermotropic nematic (3a: isotropic → nematic 160 °C DSC; nematic → isotropic 170 °C → nematic 149 °C, evidenced by polarizing microscopy, cooling. 3b: 194 °C polarizing microscopy, cooling isotropic → nematic), both displaying Schlieren textures. Copolymer 3c displays a broad halo at 4.3 Å, and a weak small angle feature, suggesting either small domain sizes or a disordered structure. No identifiable textures develop upon thermal treatment. Only in the case of 3a is the isotropic → nematic transition observed in the DSC and it is exothermic, with 0.27 kcal mol−1 per repeating unit, a small but not unexpected value.11 Polymer 3d is crystalline and does not show any phase transition up to 300 °C.
In conclusion we have presented the synthesis and characterization of a new series of liquid-crystalline PPE copolymers 3 which exhibit blue solid state fluorescence. The blue shift increases with the amount of naphthalene. Particularly attractive is the intensity of luminescence of 3 in the solid state. The increased solid-state fluorescence is attributed to the absence of aggregates and excimers, which normally reduce PPE’s quantum efficiencies of emission in the solid state. Application of 3 in LEDs and sensory materials12 is currently being explored.
Footnote |
† Sample coploymerization: 1 (0.35 g, 0.71 mmol), 2 (0.24 g, 0.71 mmol), Mo(CO)6 (0.034 g, 0.07 mmol), 4-chlorophenol (0.091 g, 0.71 mmol) and 1,2-dichlorobenzene (20 mL) were held at 140 °C under a steady stream of N2 for 17 h. Addition of chloroform acid and base washes and precipitation into methanol furnish 3c in 80% yield. Selected data for 3c: δH 8.58–8.54 (m), 8.07 (br s), 7.94 (br s), 7.60–7.42 (m), 3.02–2.89 (m), 2.13 (br s), 2.12 (br s), 1.79–1.68 (m), 1.51–1.22 (m), 0.88–0.87 (br s); δC 148.4, 141.9, 132.5, 131.3, 123.0, 122.8, 121.1, 93.5, 92.7, 35.1, 34.4, 32.0, 31.4, 31.3, 30.8, 29.8, 29.5, 29.4, 22.8, 14.2; νmax(KBr)/cm−1 3444, 2957, 2923, 2853, 2350, 1651, 1463, 1384, 1025, 886, 771. |
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