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1.
白永林  韦玮  刘俊锋 《发光学报》2003,24(5):465-468
用脱氯化氢法制备了可溶性烷氧取代聚对苯乙炔衍生物,聚(2-甲氧基—5—丁氧基)对苯乙炔(PMOBOPV)、聚(2—甲氧基—5—辛氧基)对苯乙炔(PMOOOPV),该反应具有较高的产率,并且产品具有很好的溶解性和成膜性,同时对其薄膜进行了扫描电镜分析。利用所合成的:PPV衍生物制作了单层及不同结构的多层器件,测试了它们的电致发光性质,同时研究了不同条件对器件的起亮电压、稳定性的影响。结果表明,所制作的器件具有较好的稳定性,单层器件的起亮电压约为4V,发光峰在580nm处。  相似文献   

2.
李宝铭  吴洪才  李晓奇  易文辉 《光子学报》2006,35(10):1522-1525
通过双醚化反应、氯甲基化反应以及在强碱性条件下进行的脱氯化氢反应制备聚(2-甲氧基-5-丁氧基)对苯乙炔(PMOBOPV)、聚(2-甲氧基-5-己氧基)对苯乙炔(PMOHOPV)、聚(2,5-二丁氧基)对苯乙炔(PDBOPV)和聚(2,5-二己氧基)对苯乙炔(PDHOPV)等四种可溶性聚对苯乙炔(PPV)衍生物,通过紫外-可见吸收光谱对产物分子结构进行表征.结果显示,PMOBOPV、PMOHOPV、PDBOPV和PDHOPV的共轭π电子发生π → π* 跃迁的吸收峰分别位于491 nm、495nm、504nm和510nm处,相应的光学禁带宽度分别为2.23eV、2.18eV、2.12eV和2.07eV.利用简并四波混频技术测量PPV衍生物的三阶非线性光学性能,探讨了分子结构对PPV衍生物三阶非线性极化率(χ(3))的影响.研究发现,激发波长为532 nm时,PMOBOPV、PMOHOPV、PDBOPV和PDHOPV的共振χ(3)值分别为3.45×10-10、5.13×10-10、7.15×10-10和9.61×10-10 esu;激发波长为1064 nm时,它们的非共振χ(3)值分别为1.09×10-11、1.42×10-11、1.62×10-11和2.14×10-11 esu.  相似文献   

3.
基于碳纳米管的良好导电性、激子传输性能和量子点聚合物复合材料高的光电转换性能,采用原位缩合法制备了聚合物聚(2-甲氧基-5-辛氧基)-对苯乙炔-功能化碳纳米管-硒化铅量子点复合材料.通过对复合材料的X射线衍射、透射电子显微镜和紫外可见吸收光谱研究,发现聚合物聚(2-甲氧基-5-辛氧基)-对苯乙炔,功能化碳纳米管与硒化铅量子点可以有效地复合,且功能化碳纳米管与聚合物聚(2-甲氧基-5-辛氧基)-对苯乙炔形成网状结构;硒化铅量子点尺寸为5.75nm,其可均匀地分散在聚合物聚(2-甲氧基-5-辛氧基)-对苯乙炔-功能化碳纳米管基体中形成包覆或镶嵌结构,并发生了光诱导电荷转移.通过对复合材料的光电性能研究发现,插入不同厚度阴极修饰材料LiF后其光电性能提高,且当LiF为3nm时,开路电压为0.558 V,短路电流为2.338 mA,填充因子为37.6%,转换效率为0.466%,与不插入修饰材料时相比复合材料光电性能提高了30%.  相似文献   

4.
制备了一种基于荧光聚合物共混的单发光层聚合物白光发光二极管.器件结构为铟锡氧化物/苯磺酸掺杂聚乙烯基二氧噻吩/发光层/ 1,3,5-三(N-苯基-2-苯并咪唑-2)苯41/Ba/Al,蓝光材料芴-氟化喹喔啉共聚物(PF-BPFQ5)、绿光材料苯基取代的聚对苯乙炔(P-PPV)和红光材料聚(2-甲氧基-5-(2′-乙基己氧基)-1,4-对苯乙炔)(MEH-PPV)共混为发光层.当PF-BPFQ5,P-PPV,MEH-PPV的质量比例为100∶06∶06时,获得标准的白光,色坐标为(033 关键词: 聚合物发光二极管 白光 共混  相似文献   

5.
采用吸收光谱、荧光光谱和皮秒Z-扫描等实验方法研究了侧链长度的不同对聚[2-甲氧基-5-(2′-乙基-己氧基)]对苯乙炔(MEH-PPV)和聚(2,5-二辛氧基)对苯乙炔(DO-PPV)两种聚对苯乙炔(PPV)衍生物光学性质的影响,并用π-电子共轭结构理论和共振、非共振增强理论进行了分析。结果表明,侧链较长的MEH-PPV的吸收峰和荧光发射峰比DO-PPV相应的吸收和荧光峰均有所红移;侧链结构及共振增强使得MEH-PPV的三阶非线性极化率比DO-PPV增强了近两个量级,并在532 nm激发时,χ(3)具有最大值9.30×10-10esu。  相似文献   

6.
纳米MEH-PPV阵列的光致发光   总被引:1,自引:1,他引:0  
以多孔氧化铝为模板,将可溶性发光聚合物聚(2-甲氧基-5-(2’-乙基己氧基)-1,4-对苯乙炔)(MEH-PPV)镶嵌在纳米孔中,制备出高发光效率的纳米发光聚合物阵列,其光学特性与MEH-PPV薄膜显著不同。纳米孔内的MEH-PPV分子链形成链束,链束中的分子链数目依赖于制备纳米MEH-PPV阵列所用溶液的浓度。相对于稀溶液,在由浓溶液制备的纳米MEH-PPV阵列中,MEH—PPV链束的分子链数目较多,链间作用使MEH-PPV的能带展宽,能隙减小,因而浓溶液获得的纳米MEH—PPV阵列的光致发光峰红移。热处理纳米MEH-PPV阵列的PL谱表明,纳米孔内的聚合物分子链的弛豫运动受到限制。  相似文献   

7.
本文对以聚(2,5-二丁氧基对苯乙炔)为发光层的聚合物电致发光二极管的电致发光性能和影响其性能的因素进行了研究.其发光峰值波长为590um,起亮电压为12V,最大亮度可达112cd/m2.热处理温度和时间影响其发光强度和峰值波长,一般以200℃,真空处理3.5h为宜.还原气氛(N2+H2)下的热处理有利于电致发光性能的提高.器件在空气中具有一定的使用寿命.其量子效率可达0.16%光子/电子.并研究了器件制备工艺对性能的影响,初步探讨了聚合物电致发光机理.  相似文献   

8.
一种压控波长可调谐异质结有机薄膜发光二极管   总被引:2,自引:0,他引:2  
谭海曙 《光学学报》1998,18(7):38-942
利用空穴型聚合物材料ROPPV-12[聚(十二烷氧基-对苯乙炔)]与电子型有机小分子材料Alq3(八羟基喹啉铝)配合制备了有机薄膜异质结发光二极管。发现该异质结器件在ROPPV-12的厚度保持为70nm、Alq3的厚度为20nm时,器件的性能最优,且电致发光完全来自ROPPV-12;而当Alq3的厚度为32nm时,发光区域则跨越了ROPPV-12与Alq3,器件在较低驱动电压下来自ROPPV-12的光发射占主导地位,随着电压的升高,Alq3的光发射逐渐占据了主导地位。在相同电压下,前一器件的亮度、电流、发光效率都要远高于后一器件。分析了其发光机理。  相似文献   

9.
分别采用紫外光电子能谱(UPS)、X光电子能谱(XPS)、原子力显微镜(AFM)、以及光致发光光谱(PL)等方法对在大气存放条件下的8-羟基喹啉铝(Alq)薄膜和聚(9,9-二辛烷基芴)(PFO)薄膜的电子结构、表面形 及发光特性进行了对比。研究结果表明,PFO的电子结构、表面形貌以及发光特性受外界气氛影响极小,是一种非常稳定的聚合物发光材料。这为聚合物发光器件的稳定性提供了有利的条件。  相似文献   

10.
近年来,聚对苯乙炔(PPV)及其衍生物作为一类性能优良的电致发光材料而受到人们的广泛关注[1].这是因为聚合物发光材料能通过化学裁剪方法来改善发光效率、颜色、成膜性等特性.载流子形成激子以及激子的辐射和非辐射衰减过程向来是聚合物发光二极管(LEDs)发光的重要环节,因此研究聚合物的光物理过程对提高器件的发光特性是非常重要的.  相似文献   

11.
Two-dimensional scanning of a 0.6328 mum guided-light beam has been realized using noncolinear acousto-optic (AO) coplanar Bragg diffraction together with colinear AO guided-mode to substrate radiation-mode conversion in a Z-cut Xpropagation LiNbO3 proton-exchanged (PE) waveguide. The two surface acoustic (SAW) waves utilized are at the center frequencies of 500 and 200 MHz, propagating in the Y and X axes, respectively. Two-dimensional scanning of approximately 720 resolvable light beam spots, namely, 18 40 (horizontal vertical) scanning, has been demonstrated using a light beam of 1.0 mm aperture. The total number of resolvable beam spots can be greatly increased from 720 by simply utilizing SAW transducers of larger bandwidth and a light beam of greater aperture. It should also be possible to significantly increase the diffraction efficiency from 3 % by optimizing the parameters of the PE waveguide and the SAWs.  相似文献   

12.
Results of a study of the effect of γ-radiation on the spectral luminescence properties of cadmium tungstate crystals doped with silver, bismuth, and molybdenum cations are presented. Spectral characteristics of the nondnnnoped crystals are briefly described. Absorption and photo and X-ray luminescence spectra of the crystals taken before and after exposure to γ-radiation (5.5·104 Gy) are compared. It is found that the spectral characteristics of the crystals doped with silver, bismuth, and molybdenum cations do not change markedly after the exposure. The relation between the type of impurity-induced defects, individual characteristics of the impurity cations, and the character of the effect of γ-radiation on the spectral luminescence properties of impure crystals is analyzed (preliminarily). Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 64, No. 1, pp. 55–60, January–February, 1997.  相似文献   

13.
We measure the waveform and phase curves of short optical pulses before and after transmission over different lengths of fibers by use of the pulse analyzer with the frequency-resolved optical gating (FROG),and numerically simulate pulse evolution under the experimental conditions.The nonlinear coefficient of the fiber is given by comparing the experimental results with the numerical ones.Difference between the experiment and numerical simulation is analyzed.  相似文献   

14.
Resonance scattering of elastic spherical shell and cylindrical shell while the surrounding fluid medium has absorption is studied. The normal mode solution derived using exact elastic theory and the separation of variables is still applicable. However, the scattering form function has to be modified for the absorbing medium, otherwise the unreasonable result would be obtained. The backscattering form function in the absorbing medium is redefined, and the form function of elastic spherical and cylindrical shell with vacuum or solid matter filled is calculated in various absorption conditions. The results show that the absorption of surrounding fluid leads to notable attenuation of the coincidence resonances in the mid-frequency, but it has a little influence on the low-frequency resonance scattering induced by the filler inside the shell.  相似文献   

15.
A versatile and low-cost single-beam self-referenced phase-sensitive surface plasmon resonance(SPR)sensing system with ultra-high resolution performance is presented.The system exhibits a root-mean-square phase fluctuation of ±0.0028.over a period of 45 min.i.e.a resolution of±5.2×10-9 refractive index units.The enhanced performance has been achieved through the incorporation of three design elements:a true single-beam configuration enabling complete self-referencing so that only the phase change associated with SPR gets detected,a differential measurement scheme to eliminate spurious signals not related to the sensor response,and the elimination of retardation drifts by incorporating temperature stabilization in the liquid crystal phase modulato .Our design should bring the detection sensitivity of non-labeling SPR biosensing closer to that achievable by conventional fluorescence-based techniques.  相似文献   

16.
Ta2O5 films are prepared on BK7 substrates with conventional electron beam evaporation deposition.The effects of SiO2 protective layers and annealing on the laser-induced damage threshold (LIDT) of the films are investigated.The results show that SiO2 protective layers exert little influence on the electric field intensity(EFI)distribution,microstructure and microdefect density but increase the absorption slightly.Annealing iS effective on decreasing the microdefect density and the absorption of the films.Both SiO2 protective layers and annealing are beneficial to the damage resistance of the films and the latter is more effective to improve the LIDT.Moreover,the maximal LIDT of Ta2O5 films is achieved by the combination of SiO2 protective layers and annealing.  相似文献   

17.
Gray cross correlation matching technique is adopted to extract candidate matches with gray cross correla- tion coefficients less than some certain range of maximal correlation coefficient called multi-peak candidate matches. Multi-peak candidates are extracted corresponding to three closest feature points at first. The corresponding multi-peak candidate matches are used to construct the model polygon. Correspondence is determined based on the local geometric relations between the three feature points and the multi-peak candidates. The disparity test and the global consistency checkout are applied to eliminate the remaining ambiguous matches that are not removed by the local geometric relational test. Experimental results show that the proposed algorithm is feasible and accurate.  相似文献   

18.
A novel method based on fiber gratings for measuring the effective indices of fiber modes is proposed. The effective index difference between the core mode and a cladding mode was obtained by analyzing the interference fringe of a pair of cascaded long-period fiber gratings. In order to extract the core mode index from the measured index difference, an index matching oil immersion method is proposed. By analyzing the interaction between the cladding mode and the oil applied on the cladding surface, the mode order and the effective index of the involved cladding mode might be calculated. Experimental results about the interference fringe shifts induced by the oil index and the oil-applied length are also presented.  相似文献   

19.
Optical Pulse Compression Schemes That Use Nonlinear Bragg Gratings   总被引:2,自引:0,他引:2  
Nonlinear optical pulse compression of picosecond pulses typically requires long lengths of optical fiber and multiple components. Periodic structures, such as fiber Bragg gratings, are highly dispersive at wavelengths outside of the photonic bandgap. This implies that such gratings can be used as very short all-fiber compressors. In this paper a number of such compression schemes are reviewed involving uniform and nonuniform fiber Bragg gratings, relying on both soliton and nonsoliton compression principles. Experimental results supporting the corresponding underlying theory are also presented. Finally, an extension of one of the compression schemes is shown, which allows the generation of adjustable high-repetition rate soliton trains.  相似文献   

20.
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