Influence of molecular weight on the phase behavior and structure formation of branched side-chain hairy-rod polyfluorene in bulk phase -: art. no. 041802

被引:55
作者
Knaapila, M
Stepanyan, R
Torkkeli, M
Lyons, BP
Ikonen, TP
Almásy, L
Foreman, JP
Serimaa, R
Güntner, R
Scherf, U
Monkman, AP
机构
[1] Univ Durham, Dept Phys, Durham DH1 3LE, England
[2] Univ Twente, Dept Appl Phys, NL-7500 AE Enschede, Netherlands
[3] Univ Helsinki, Dept Phys Sci, FI-00014 Helsinki, Finland
[4] Res Inst Solid State Phys & Opt, H-1525 Budapest, Hungary
[5] Berg Univ Wuppertal, Inst Polymertechnol, D-42097 Wuppertal, Germany
来源
PHYSICAL REVIEW E | 2005年 / 71卷 / 04期
关键词
D O I
10.1103/PhysRevE.71.041802
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
We report on an experimental study of the self-organization and phase behavior of hairy-rod pi-conjugated branched side-chain polyfluorene, poly[9,9-bis(2-ethylhexyl)-fluorene-2,7-diyl]-i.e., poly[2,7-(9,9-bis(2-ethylhexyl)fluorene] (PF2/6)-as a function of molecular weight (M-n). The results have been compared to those of phenomenological theory. Samples for which M-n=3-147 kg/mol were used. First, the stiffness of PF2/6, the assumption of the theory, has been probed by small-angle neutron scattering in solution. Thermogravimetry has been used to show that PF2/6 is thermally stable over the conditions studied. Second, the existence of nematic and hexagonal phases has been phenomenologically identified for lower and higher M-n (LMW, M-n < M-n(*) and HMW, M-n>M-n(*)) regimes, respectively, based on free-energy argument of nematic and hexagonal hairy rods and found to correspond to the experimental x-ray diffraction (XRD) results for PF2/6. By using the lattice parameters of PF2/6 as an experimental input, the nematic-hexagonal transition has been predicted in the vicinity of glassification temperature (T-g) of PF2/6. Then, by taking the orientation parts of the free energies into account the nematic-hexagonal transition has been calculated as a function of temperature and M-n and a phase diagram has been formed. Below T-g of 80 degrees C only (frozen) nematic phase is observed for M-n < M-n(*)=10(4) g/mol and crystalline hexagonal phase for M-n>M-n(*). The nematic-hexagonal transition upon heating is observed for the HMW regime depending weakly on M-n, being at 140-165 degrees C for M-n>M-n(*). Third, the phase behavior and structure formation as a function of M-n have been probed using powder and fiber XRD and differential scanning calorimetry and reasonable semiquantitative agreement with theory has been found for M-n >= 3 kg/mol. Fourth, structural characteristics are widely discussed. The nematic phase of LMW materials has been observed to be denser than high-temperature nematic phase of HMW compounds. The hexagonal phase has been found to be paracrystalline in the (ab0) plane but a genuine crystal meridionally. We also find that all these materials including the shortest 10-mer possess the formerly observed rigid five-helix hairy-rod molecular structure.
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页数:13
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