Persistence of Nematic Liquid Crystalline Phase in a Polyfluorene-Based Organic Semiconductor: A High Pressure Study

被引:5
|
作者
Guha, Suchismita [1 ]
Knaapila, Matti [2 ]
Moghe, Dhanashree [1 ]
Konopkova, Zuzana [3 ]
Torkkeli, Mika [4 ]
Fritsch, Martin [5 ]
Scherf, Ullrich [5 ]
机构
[1] Univ Missouri, Dept Phys & Astron, Columbia, MO 65211 USA
[2] Inst Energy Technol, Dept Phys, NO-2027 Kjeller, Norway
[3] Photon Sci DESY, D-22607 Hamburg, Germany
[4] Univ Helsinki, Dept Phys, FI-00014 Helsinki, Finland
[5] Berg Univ Wuppertal, Macromol Chem Grp, D-42097 Wuppertal, Germany
关键词
conjugated polymers; fluorescence; liquid-crystalline polymers; X-ray; STRUCTURE-PROPERTY RELATIONSHIPS; LIGHT-EMITTING-DIODES; MOLECULAR-WEIGHT; HYDROSTATIC-PRESSURE; DEVICE APPLICATIONS; MORPHOLOGY; PACKING; ELECTROLUMINESCENCE; OLIGOFLUORENES; CONFORMATION;
D O I
10.1002/polb.23520
中图分类号
O63 [高分子化学(高聚物)];
学科分类号
070305 ; 080501 ; 081704 ;
摘要
The role of high pressure on a low molecular weight nematic liquid crystalline organic semiconductor, ethylhexyl substituted polyfluorene (PF2/6) is investigated using photoluminescence (PL), Raman scattering, and X-ray scattering studies at pressures from 1 to 8 GPa. The PL and the Raman data under pressure are consistent with each other with no abrupt changes in the pressure coefficients of PL or Raman peaks. The PL energies redshift and broaden, consistent with both enhanced intra-and interchain interactions. The Raman peak positions yield pressure coefficients similar to other phenyl based p-conjugated polymers. The broadening of a doublet peak in the 1135 cm 21 region indicates a more planar backbone conformation with increasing pressure. X-ray scattering indicates that the torsion angle between adjacent repeats reduces with increasing pressure and reverts back with decompression. The intermolecular structure is weakly ordered (frozen nematic) and essentially maintained with increasing pressure, in contrast to a high molecular weight PF2/6. (C) 2014 Wiley Periodicals, Inc.
引用
收藏
页码:1014 / 1023
页数:10
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