电子传输层厚度对LiBq4蓝色有机电致发光器件的影响

制备了以LiBq4为发光层,结构为ITO/CuPc/TPD/LiBq4/Alq3/LiF/Al的器件.器件的电致发光(EL)光谱与LiBq4薄膜的光致发光(PL)光谱相同,峰值波长均为492nm.改变电子传输层Alq3的厚度时,器件的电流-电压特性及发光光谱随之发生变化,当电子传输层的厚度为5nm时,既可以避免电子传输层的发光,又可以降低器件的工作电压.     

多层结构对有机电致发光器件性能的影响

将发光层进行多次堆叠,构造出有机电致发光器件.在堆叠过程中,改变各发光层厚度的相对比例,发现在总厚度相同、结构相同,而各发光层比例不同的条件下,器件呈现不同的发光特性.器件的电致发光光谱有着明显的变化,器件颜色由蓝光到近白光改变极其明显,器件的亮度和器件的效率也有不同程度的改变.     

芴类衍生物有机电致发光器件中的激基复合物

利用紫外-可见光吸收光谱和荧光发光(PL)光谱,研究了新型芴类小分子材料2,3-bis(9,9-dihexyl-9H-flu-oren-2-yl)-6,7-difluoroquinoxaline(F2Py)的本征光谱特性,并制备了基于F2Py的有机电致发光器件(OLEDs),讨论了器件的电致发光(EL)光谱。结果表明,F2Py在溶液状态下的本征PL峰值位于452 nm,在薄膜状态下的本征PL峰值位于448 nm,而F2Py与NPB的混合物的PL发光峰在544 nm。在器件的EL光谱中,观察到了位于530~550 nm范围的激基复合物发光峰,以及来自F2Py与NPB激子发光的共同作用形成的位于430nm左右的肩峰。当F2Py层厚度为50 nm时,器件的启亮电压为17 V,最高亮度为58 cd/m2;而当F2Py厚度为20 nm并加入了Alq3(10 nm)做电子传输层(ETL)时,器件启亮电压为8 V,最高亮度为5030 cd/m2,EL性能大大提高。     

NPB/Alq3双层有机电致发光器件薄膜厚度与器件性能的优化

研究了以NPB为空穴传输层、Alq₃为发光层的双层异质结有机电致发光器件的薄膜厚度对器件性能的影响.制备了一系列具有不同NPB和Alq₃厚度的器件并测试了其电致发光特性.结果表明,器件电流随Alq₃与NPB厚度变化的关系并不相同.不同有机层厚度双层器件的电流机制符合陷阱电荷限制(TCL)理论,随外加电压的增大,器件电流经历了欧姆电导区、TCL电流区、陷阱电荷限制-空间电荷限制(TCL-SCL)过渡区三个区域的变化.当有机层厚度匹配为NPB(20nm)/Alq₃(50nm)时可以获得性能优良的器件.器件的流明效率-电压关系曲线的变化规律是在低电压区较快达到最大值,然后随电压的增加逐渐降低.     

NPB蓝色有机电致发光器件的性能优化研究

基于结构为ITO/NPB/BCP/Alq3/Mg:Ag的NPB(N,N’-bis(1-naphthyl)-N,N’-diphenyl-1,1’-biphenyl-4,4’-diamine)蓝色有机电致发光器件,利用Alq3的空穴阻挡能力及高的荧光效率优化了器件结构。具有不同厚度Alq3空穴阻挡层的器件性能测试结果表明,Alq3对器件发光亮度影响明显,选择适当的Alq3厚度可使得器件的发光亮度提高大约两倍。电致发光光谱测试结果表明,器件的发光基本来自NPB的蓝色发光,而Alq3扮演了辅助发光层的作用。     

SrS:CeCl_3薄膜的高亮度蓝色EL

用于薄膜电致发光(EL)器件的 SrS:CeCl_3发光层的结晶性能直接受与其邻近的底层膜的影响。在一种以强立方(111)取向 ZnS 薄膜作为底层的 EL 薄膜器件中实现了明亮的蓝色发射,在5KHz 正弦电压激发下,器件的最大亮度力100nt。根据 x 射线衍射图和发光层的光致发光光谱讨论了 EL特性。     

BCP层对蓝光有机电致发光器件效率的影响

采用真空热沉积的方法,在常规的三层器件基础上,通过改变空穴阻挡层BCP的厚度,制备了具有结构为氧化铟锡(ITO)/N,N'-diphenyl-N,N'-bis(1-naphthyl)(1,1'-biphenyl)-4,4'-diamine(NPB)/2,9-dimethyl-4,7-diphenyl-1,10-phenan throline(BCP)/Hydroxyquinoline aluminum(Alq3)/Mg:Ag的双异质结的有机电致发光器件.结果表明,当空穴阻挡层BCP的厚度从0.1 nm逐渐增加到4.0 nm时,器件的电致发光光谱实现了从绿色到蓝绿色再到蓝色发射的转变.同时,空穴阻挡层BCP起到了调节载流子复合区域和改变器件发光颜色的作用,并且通过详细的器件结构优化证明一定厚度的BCP层显著地提高了蓝光器件的效率,达到了7.3 lm/W.     

有机小分子掺杂的聚合物发光二极管电致发光及其发射机制

在新型空穴传输聚合物聚TPD(PTPD)中掺杂电子传输有机小分子荧光染料Rubrene制成薄膜器件.考察了影响聚合物掺杂小分子薄膜器件发光性能的因素.实验表明,通过在器件中掺杂,可以控制器件所发光的颜色.研究了PTPD掺杂Rubrene分子薄膜的电致发光光谱和光致发光光谱.由实验可知.在光致发光中存在从PTPD向Rubrene的能量传递和电荷转移,而电致发光则存在从PTPD向Rubrene的能量传递和Rubrene分子对载流子的俘获.即掺杂器件的发射机制为载流子陷阱和Forster能量转换过程的共同作用.     

有空穴传输层的双层有机薄膜电致发光器件

制备了由有机空穴传输层和有机发光层组成的双层有机薄膜电致发光器件,器件的发光亮度相对于单层器件有了很大的提高。并用不同深度区域的掺杂方法,对其电致发光机理作了探讨。对单、双层器件的不同的亮度电流关系、不同的发光区域进行了分析和讨论.     

有机小分子掺杂的聚合物发光二极管电致发光及其发射机制

在新型空穴传输聚合物聚TPD(PTPD)中掺杂电子传输有机小分子荧光染料Rubrene制成薄膜器件.考察了影响聚合物掺杂小分子薄膜器件发光性能的因素.实验表明,通过在器件中掺杂,可以控制器件所发光的颜色.研究了PTPD掺杂Rubrene分子薄膜的电致发光光谱和光致发光光谱.由实验可知.在光致发光中存在从PTPD向Rubrene的能量传递和电荷转移,而电致发光则存在从PTPD向Rubrene的能量传递和Rubrene分子对载流子的俘获.即掺杂器件的发射机制为载流子陷阱和Forster能量转换过程的共同作用.     

多孔硅中八羟基吡啉铝的光致发光

通过两种方法将有机小分子八羟基喹啉铝（Alq3)嵌入到用阳极腐蚀法制备的多孔硅中。一是浸泡法,将新鲜的多孔硅浸泡于Alq3的氯仿溶液中,通过物理吸附使Alq3嵌入到多孔硅的纳米孔中;二是反应法,先将多孔硅浸泡于硫酸铝的水溶液中,再在其中加入八羟基喹啉的甲醇溶液,使它们在多孔硅的纳米孔中反应产生Alq3。两种方法得到的Alq3的光致发光光谱均较硅片上蒸镀的Alq3的光致发光光谱有所蓝移,半高宽有所减小。反应法比浸泡法得到的光致发光强得多。     

Polymer Films with Metal-Like Thermal Conductivity,Excellent Stability,and Flame Retardancy

Polymers often have thermal conductivities that are too low to be used directly in thermal management applications. In this study, a poly(p-phenylene-2,6-benzobisoxazole) (PBO) film is prepared through a sol–gel-film conversion and annealing method that utilizes PBO nanofibers as building blocks. The polymer film shows an in-plane thermal conductivity of 36.7 W mK⁻¹, which is two orders of magnitude higher than those of most polymers (<0.5 W mK⁻¹) and 2.4 times that of 304-stainless steel. The high thermal conductivity is attributed to the highly oriented 3D interconnected nanofiber network resulting from the fine-tuning sol-gel-film conversion, and the annealing that further enhances the ordering of the PBO chains and the interactions between the nanofibers. Moreover, the PBO films exhibit excellent mechanical strength, thermal/chemical stability, electrical insulation, flame retardance, and improved UV resistance. The lightweight, robust, and easily processed PBO film with a metal-like thermal conductivity has promising potential thermal management applications.     

有机白光LED

有机白光LED主要有电致发光与光致发光两类。电致发光的主要机理有:量子阱发光、激基复合物发光和能量转移。人们对有机电致发光白光LED研究较多,不久将有产品问世;而对光致发光研究较少。与电致发光相比,光致发光造价更小,其荧光量子效率或许比电致发光更高。有机白光LED制备工艺简单、成本低功耗小,具有巨大的应用价值及潜在的市场。对发光显示技术,有机白光LED代表了一条“便宜”经济的路径。综述了有机白光LED的机理及发展现状。     

Molecular packing correlated fluorescence in TIPS-pentacene films

The molecular packing and optical properties of exposed and buried layers (i.e. the layers at the top surface and near the substrate, respectively) were systematically studied in 6,13-Bis(triisopropylsilylethynyl)pentacene (TIPS-pentacene) films coated by spin-coated (SC) and droplet-pinned-crystallization (DPC) methods. Buried layers in both films exhibit intense photoluminescence (PL) resembling the behaviors of the molecules in dilute solution ascribing to weak π-π stacking, while the exposed layers show extremely weak PL due to strong crystallinity. Polarized excitation PL spectra demonstrate that molecular orientation of the buried layers is quasi-ordered in the film coated by DPC method and completely disordered in the film coated by SC method. Besides, the strong crystallinity of the exposed TIPS-pentacene is verified by grazing incident wide-angle X-ray scattering measurement. The distinct differences in optical and structural properties between the exposed and buried layers indicate that TIPS-pentacene films are inhomogeneous in vertical direction due to interfacial effect, which affects the performance of photodiode fabricated with both films. The understanding of the molecular packing correlated fluorescence in TIPS-pentacene films is vital for optimizing the film structure to achieve high performance organic electronic devices.     

Optimization of the Luminescence Efficiencies in Solution-Processed Phosphorescent Dendrimers

We demonstrate that photoluminescence (PL) quantum yield and PL lifetime of fac-tris(2-phenylpyridyl) iridium(III) [Ir(ppy)₃]-cored dendrimers in neat film and dispersed into a 4,4'-bis(N-carbazolyl)biphenyl host can be significantly improved by a simple adjustment of the solution preparation. Quenching of the PL in these materials is due to an energy transfer of the triplet excitons to less-emissive sites and can be reduced by blending the phosphorescent molecules into a suitable wide energy gap host or by increasing the number of attached dendrons. We show here that the concentration of these quenchers can also be controlled by changing the time spent by the dendrimer solution under illumination prior to spin-coating. By optimizing the film preparation procedure, the external efficiency of devices made from neat dendrimer films was increased from 2% to 10%     

CdSe四脚状纳米晶粒的光荧光研究

采用高温微乳液的化学方法,在溶液中合成了高产率的CdSe四脚状纳米晶粒。高分辨透射电镜(HRTEM)分析结果表明,CdSe四脚状纳米晶粒是由1个立方的核心和4个六方的臂所组成。研究了该四脚晶粒的变激发功率光荧光(PL)谱和变温的PL谱,分析发现低温时四脚晶粒的光荧光主要来自于被表面缺陷所局域的激子的辐射复合,而随着温度升高,束缚激子被热激发,室温时光荧光主要来自于自由激子的贡献。CdSe纳米量子点的退局域化温度比四脚纳米晶粒的高,而12K时CdSe纳米量子点的局域化能量比四脚纳米晶粒的也大得多,并对这一现象作了解释。     

溅射ZnO薄膜钝化GaAs表面性能的研究

为了改善GaAs(110)与自身 氧化物界面由于高表面态密度而引起的费米能级钉扎(pinning)问题 ,提出采用射频磁控溅射技 术在GaAs(110)衬底上沉积一定厚度 ZnO薄膜作为钝化层,并利用光 致发光(PL)光谱和X射线光电子能谱(XPS) 等方法对ZnO薄膜的光学特性及钝化性能进行表征。实验结果表明,经ZnO薄膜钝化后的 GaAs样品,其本征PL峰强度提高112.5%,杂质峰强度下降82.4%。XPS光谱分析表明,Ga和As原子的比值从1.47降低 到0.94,ZnO钝化层能 够抑制Ga和As的氧化物形成。因此,在GaAs表面沉积ZnO薄膜是一种可行的GaAs表面钝化 方法。     

Gaq3有机薄膜电致发光器件

首次报道了采用８－羟基喹啉镓螯合物作为发光层制备有机薄膜电致发光器件，器件的结构为：ＩＴＯ导电玻璃／ＴＰＤ／Ｇａｑ３／Ａｌ。研究了Ｇａｑ３薄膜的光致发光和器件的电致发光机理，同时测量和研究了器件的电流密度－－电压（Ｊ－Ｖ）特性和发光亮度－电压（Ｂ－Ｖ）特性。结果表明器件的电致发光峰值波长为５４０ｎｍ，在２０Ｖ直流电压驱动下的最大发光亮度约２５００ｃｄ／ｍ＾２明显高于上同结构和工艺参数制备的Ａｌｑ３     

ZnO growth on Si with low-temperature CdO and ZnO buffer layers by molecular-beam epitaxy

Low-temperature (LT) buffer-layer techniques were employed to improve the crystalline quality of ZnO films grown by molecular-beam epitaxy (MBE). Photoluminescence (PL) spectra show that CdO, as a hetero-buffer layer with a rock-salt structure, does not improve the quality of ZnO film grown on top. However, by using ZnO as a homo-buffer layer, the crystalline quality can be greatly enhanced, as indicated by PL, atomic force microscopy (AFM), x-ray diffraction (XRD), and Raman scattering. Moreover, the buffer layer grown at 450°C is found to be the best template to further improve the quality of top ZnO film. The mechanisms behind this result are the strong interactions between point defects and threading dislocations in the ZnO buffer layer.