聚芴共轭聚合物在稀薄溶液中形态变化的静态光散射研究

PF8聚芴共轭高分子材料是应用于制作蓝色光激发光器件的一种有潜力功能材料, 故本文利用静态光散射技术研究了PF8聚芴共轭高分子在稀薄甲苯溶液中的形态结构变化特点。研究结果显示, PF8共轭高分子在甲苯稀薄溶液中单一分子链的持续长度与Kuhn链结长度均明显受到温度的影响。这表明在较高温度下高分子与溶剂间的相互作用力较大, 导致其呈现较伸展的虫状形态结构; 而在较低温度下高分子与溶剂间相互作用力较小, 导致其呈现收缩的结构形态。因此在较高温度状态下PF8共轭高分子应该具有比较刚硬的特征。     

共轭聚合物链中光激发过程的无序效应

应用包含链内无序和电子关联的Su-Schriffer-Heeger模型,研究了共轭聚合物链中无序效应在光激发演化过程中的作用,尤其是对激子产率的影响.采用multi-configurational time-dependent Hartree-Fock方法处理电子部分的含时Schr?dinger方程,而晶格部分的运动则...     

苯-烷氧基苯有机共轭聚合物的光致发光性能

介绍了4种新型发光材料苯—烷氧基苯共聚物的合成方法。材料的UV—Vis吸收光谱及其薄膜和溶液的光致发光性能。用电化学掺杂方法测定了其能带结构。并讨论了烷氧基侧基长度对高聚物发光强度的影响。结果表明，这4种高聚物在紫外光激发下均发蓝光，π-π^*跃迁(Eg)值为3．2～3．3eV，烷氧基中碳原子数为10个左右时发光强度最高。     

具有共轭结构的导电聚合物及其应用

具有共轭结构的导电聚合物在微电子学和光电子领域有着广泛的应用前景。文章简要介绍了这类聚合物材料的主要合成方法、导电机理及其应用概况，并对目前该领域的研究进展作了扼要评述。     

高效率共轭聚合物主体绿光磷光发光二极管

因电致发光效率高和器件制备工艺简单,聚合物为主体的绿色磷光电致发光成为一个研究热点.共轭聚合物的三线态能级一般低于绿色磷光材料的三线态能级,易对磷光的发光引起猝灭导致低的发光效率,所以较少被用作绿色磷光材料的主体.通过增加聚乙烯基咔唑（PVK）作为空穴传输层,获得了高发光效率的共轭聚合物聚芴（PFO）作主体绿色磷光发射,甚至高于相同条件下以PVK为主体的绿色磷光发射.究其原因,PVK的电子阻挡作用使发光中心靠近PVK与PFO的界面,界面处PVK因为其高的三线态能级增强了绿色磷光的发光.当三-（2-苯基吡啶）-Ir（Ir（ppy）₃）掺杂浓度为2％时得到了最高的亮度效率24.8 cd/A,此时的电流密度为4.65 mA/cm²,功率效率为11 lm/W,最高亮度达到35054 cd/m²,色坐标是（0.39,0.56）. 关键词： 共轭聚合物 磷光 绿光发光     

纳米TiO2薄膜光催化氧化SO2研究

SO2是造成酸雨危害主要一种主要大气污染物，已引起公众特别是环境保护工作者的广泛关注。目前，一般采用催化燃烧、化学氧化和吸附等方法对SO2加以去除，但都还存在一定局限性，如设备投资及运行费用较高，去除不完全及有二次污染等，因此开发新型实用的环保技术是非常必要的。半导体纳米膜光催化氧化法在这方面有着突出的优点，成为近年来人们研究的热点。     

共轭聚合物单分子构象和能量转移特性研究

利用基于宽场显微光学系统的单分子散焦成像技术测量了不同构象poly[2,7-(9,9-dioctylfluorene)-alt-4,7-bis(thiophen-2-yl)benzo-2,1,3-thiadiazole](PFO-DBT)共轭聚合物单分子的光物理与动力学特性.通过分析共轭聚合物单分子的荧光轨迹和对应的发射偶极取向变化识别共轭聚合物单分子发光单元,发现延伸构象下的单分子呈现多发色团发光特性,而折叠构象下的单分子保持高效链间能量转移,呈现单个发色团发光特性.共轭聚合物单分子构象对能量转移效率的影响可用于研究基于共轭聚合物的光电器件和分子器件.     

新型共轭聚合物PFO-BT15发光二极管的电老化研究

PFO-BT15是一种电致发光中心波长为550 nm的新型共轭高分子聚合物材料,将其制成发光二极管器件,结构为ITO玻璃/聚合物PEDOT(120 nm)/有机聚合物PFO-BT15(80 nm)/Ba(4 nm)/Al(200 nm),用环氧树脂对阴极侧进行了封装,以减少氧气和水分的进入,从而影响器件的发光性能。在室温环境下对同样的器件进行不同电流密度的电老化处理,记录器件的电流电压曲线,再对老化的样品做电致发光和喇曼光谱测试。实验发现：一方面,通过器件恒定电流的大小影响器件的电压变化速度;另一方面,器件经过一定长时间的电老化,电致发光中心波长变化较小。通过啦曼光谱的测试,推断是因为PEDOT阳极的破损导致了器件的最终发光失败,而器件发光层材料的结构保持相对稳定,说明这种结构的聚合物有着相对稳定的光电性能,对于提高材料发光的稳定性提供了有价值的信息,有助于其他高效发光材料的合成以及稳定性的提高。     

SiO2包覆共轭聚合物CN-PPV纳米探针的制备与荧光性质

采用纳米沉淀法制备了半导体聚合物CN-PPV纳米粒子,并用改进的Stber方法对纳米粒子进行包覆,获得了发光稳定的SiO2/CN-PPV纳米粒子。用动态光散射(DLS)及透射电镜(TEM)方法对粒子尺寸进行了表征,结果表明包覆前的CN-PPV纳米粒子平均粒径约为30 nm,包覆获得SiO2/CN-PPV纳米粒子的平均粒径约为60 nm。通过紫外-可见吸收光谱及荧光光谱对包覆前后纳米粒子的发光性质进行了比较,发现共轭聚合物CN-PPV包覆后的发射光谱与包覆前相比发生了小的蓝移,表明共轭聚合物的分子构型可能发生了微小变化。SiO2包覆可以提高聚合物发光分子的光稳定性,并且提供用于生物分子耦联的表面,这类材料有望在生物医学成像中获得应用。     

锐钛矿型二氧化钛纳米粉体的IR光谱与光催化性能研究

采用溶胶-凝胶法制备了TiO2光催化剂,研究了不同温度下焙烧TiO2粉体的XRD和FT-IR光谱。400℃焙烧后,相应有机物的红外吸收峰消失,随着焙烧温度的升高,粉体粒径变大,800-420cm-1之间的吸收峰逐渐锐化,700℃焙烧的FT-IR谱的423cm-1为金红石型TiO2的特征Ti-O键振动。500℃焙烧的锐钛矿型TiO2粉体对水杨酸具有较好的光催化活性。     

Effective Stimulated Emission Cross-Sections of Poly(Phenylene Vinylene) Copolymers in Toluene Solution

We report optical gain measurements in four different copolymers polyp-phenylene-co-[2,5-dioctyloxy-p-phenylene-bis-2(4-nonyl phenyl) vinylene]nonyl-PpPV, polym-phenylene-co-[2,5-dioctyloxy-p-phenylene-bis-2(4-methyl phenyl) vinylene]methyl-PmPV, polyp-phenylene-co-[2,5-dioctyloxy-p-phenylene-bis-2(4-methyl-phenyl) vinylene]methyl-PpPV, polyp-phenylene-co-[2,6-naphthylene-bis-2(4-nonyl phenyl) vinylene]nonyl-PpPV-NV in toluene. The copolymers are related to poly(phenylene vinylene) and have been synthesized via Horner–Emmons polycondensation reaction. The optical gain determined from the amplified spontaneous emission (ASE) intensity is dependent on the excited stripe length. The net optical gain coefficients are found to vary between 0.1 cm^–1 in nonyl-PpPV to 2.5 cm^–1 in methyl-PmPV under nanosecond pulse excitation. The gain for Rodamine 6G was also measured under the same experimental condition and was used to determine the stimulated emission cross-sections for the four polymers and found to be _SE(peak)= 6.7 × 10^–20 cm² for nonyl-PpPV, _SE(peak)= 1.7 × 10¹⁸ cm² for methyl-PmPV, _SE(peak)= 1.4 × 10^–18 cm² for methyl-PpPV, and _SE(peak)= 1.5 × 10^–18 cm² for nonyl-PpPV-NV.     

The Electronic and Lattice Structures of the Groundand the Polaron States of Polymer Poly (Phenylene Vinylene) (PPV)

The electronic and lattice structures of poly (phenylene vinylene) (PPV) are studied theoretically. Both the electron-electron and electron-phonon interactions are taken into account in the Pariser-Parr-Pople model. The electronic band and the lattice structure of the ground state and the polaronic state are calculated by means of the unrestricted Hartree-Fock method. In the ground state, there exist eight bands in PPV including four valence bands and four conduction bands, and the benzenes can be considered to be rigid. The polaron induces the split of energy bands. There are four localized electronic states within the energy gap. The defect of the polaron appears to extend over about 5 units. The benzenes are strongly affected by the electron-phonon interaction. Our calculation for the energy band structure of the ground and polaron states are consistent with experimental absorption spectra. The results of our calculation show that the electron-phonon and inter-site electron-electron interactions play an important role in determining the electronic and lattice structures.     

The Electronic and Lattice Structures of the Ground and the Polaron States of Polymer Poly (Phenylene Vinylene) (PPV)

The electronic and lattice structures of poly (phenylene vinylene) (PPV) are studied theoretically. Both the electron-electron and electron-phonon interactions are taken into account in the Pariser-Parr-Pople model. The electronic band and the lattice structure of the ground state and the polaronic state are calculated by means of the unrestricted Hartree-Fock method. In the ground state, there exist eight bands in PPV including four valence bands and four conduction bands, and the benzenes can be considered to be rigid. The polaron induces the split of energy bands. There are four localized electronic states within the energy gap. The defect of the polaron appears to extend over about 5 units. The benzenes are strongly affected by the electron-phonon interaction. Our calculation for the energy band structure of the ground and polaron states are consistent with experimental absorption spectra. The results of our calculation show that the electron-phonon and inter-site electron-electron interactions play an important role in determining the electronic and lattice structures.     

聚合物Poly（2，5－thienyleneVinylene）中超快光学克尔效应的实验研究

实验研究了聚合物Ｐｏｌｙ（２，５－ｔｈｉｅｎｙｌｅｎｅｖｉｎｙｌｅｎｅ）薄膜的超快共振光学克尔效应。获得了３×１０－１１ｅｓｕ的光学克尔极化率。一个双激发子弛豫机制被用来解释克尔信号动力学特性对入射光强度的依赖性。     

Rheological Behavior of Blends of Poly(Phenylene Sulfide) with a Thermotropic Liquid Crystalline Aromatic Poly(Ether Ester)

A new type of thermotropic liquid crystalline aromatic poly(ether ester) (PEE) was prepared from 1,3-bis(4′-carboxyphenoxy)benzene, 1,4-diacetoxybenzene, and p-acetoxybenzoic acid through a melt transesterification process. The rheological behavior of blends of poly(phenylene sulfide) (PPS) with PEE was studied using a high-pressure capillary rheometer with the shear rate range of 50 s^?1 to 3000 s^?1. The results show that according to the range of shear rate, the flow curves of PEE/PPS blends can be divided into three zones: a first shear-thinning zone (n < 1, “n” represents non-Newtonian indexes), a shear-thickening zone (n > 1), and a second shear-thinning zone (n < 1), and the former two zones are more obvious with the increase of PEE content or elevated temperature. In the second shear-thinning zone, the PPS melt is close to a Newtonian fluid at high temperature and high shear rate; meanwhile the non-Newtonian behavior of the PPS melt at high temperature is enhanced with the addition of PEE. The apparent viscosity of PPS melts sharply dropped after adding PEE, especially at relatively low temperature and low shear rate. The curve of apparent viscosity vs. shear rate starts to flatten out after adding PEE, suggesting that the addition of PEE lowers the sensitivity of PPS to shear rate. As the content of PEE increases, the activation energy of the viscous flow, ΔE_η, of PPS decreases, which means that adding PEE weakens the temperature sensitivity of the apparent viscosity of the PPS melt. It can clearly be seen that the addition of PEE is beneficial to the processing of PPS.     

Effect of the End Groups and the Solvent on the Gelation of the Hybrid Materials from Poly (Vinyl Chloride) (PVC) and Oligo Phenylene Vinylene (OPV)

Abstract

The role of the end-groups of three oligophenylene vinylene (OPV) and the solvents on the hybrid materials from poly (vinyl chloride) (PVC) and the OPV are examined. The gelation of the three organogel OPVs and of the hybrid materials in bromobenzene and benzyl alcohol was characterized. The morphology, as well as the thermodynamic properties, of these OPV and hybrid materials showed that they depended mostly on the solvent and very little on the different end-groups located on the OPV backbones.     

聚(2-甲氧基-5-辛氧基)对苯乙炔/TiO2纳米复合材料的光物理性能研究

通过原位强碱诱导下的脱氯化氢缩合聚合法制备了一系列不同纳米TiO2含量的聚(2-甲氧基-5-辛氧基)对苯乙炔/纳米二氧化钛(PMOCOPV/TiO2)光电复合材料。红外光谱和拉曼光谱证实了在纳米TiO2表面的包覆层为PMOCOPV。紫外-可见吸收光谱表明随着TiO2含量的增加PMOCOPV/TiO2纳米复合材料的吸收强度提高。高分辨透射电镜观察发现PMOCOPV/TiO2是具有核-壳结构的纳米复合粒子,直径约30 nm,其中PMOCOPV包覆层的厚度约为8~10 nm。荧光光谱研究表明,PMOCOPV/TiO2纳米复合材料的最大发射波长随着TiO2含量的增加发生红移,荧光寿命约为1 ns,且随着TiO2含量的增加荧光强度和荧光寿命得到显著提高,并通过PMOCOPV/TiO2纳米复合材料中的激子离化和电荷传输过程以及复合材料中的电势能级探讨了PMOCOPV/TiO2的荧光量子效率和荧光强度增加的机理。     

纳米复合材料TiO2-ZrO2光催化降解可溶性染料的研究

采用溶胶-凝胶方法将光催化剂TiO2和ZrO2复合,再经700℃灼烧5h后获得了纳米复合光催化材料TiO2-ZrO2.该材料经XRD检测具有光催化活性良好的晶型结构.TEM测定结果显示产物的平均粒径约为20nm.通过对可溶性染料刚果红等的光催化降解实验证明,该复合材料具有较高的光催化活性.     

Electronic Structure of the Positive Radical of 13C-Labeled Poly(3-Octylthienylene Vinylene) Polymer

Poly(3-octylthienylene vinylene) (O-PTV) has a great potential as low-bandgap p-type semiconductor for photovoltaic applications. Here, the positive radical state (positive polaron) is induced chemically in the O-PTV polymer in which the vinylene sites are selectively ¹³C-labeled. Using multi-frequency continuous wave and pulsed electron paramagnetic resonance, the g tensor and maximum ¹H and ¹³C hyperfine couplings are determined. A comparative density functional theory (DFT) analysis of PTV-like oligomers is performed. The experimental parameters suggest a larger localization of the positive polaron than follows from the DFT analysis. The counter anion may play a crucial role in localizing the polaron.     

窄带系聚合物APFO3的激发态光物理特性 (cited: 1)

化学计算证实了光致激发窄带系聚合物APFO3后,会发生链内电荷转移(ICT)过程,同时这一特性还影响了吸收光谱中的第一吸收带. 瞬态吸收结果再一次表明了当聚合物在单分散体系中确实存在ICT特性,而且这种特性会同振动弛豫竞争. 在聚集态中,受链间相互作用的影响,ICT特性会消失,而且激子弛豫过程将在光致激发后的弛豫过程中占据主导地位. 混有PC₆₁BM的APFO3薄膜的光致激发动力学显示,当PC₆₁BM 的含量超过50%时,激子解离已经达到饱和. 基于此异质节的光