ZnSe为发光层的蓝绿光薄膜电致发光器件的发光性能

采用具有电子加速能力的Si02代替传统夹层结构中的绝缘层,利用电子束蒸发的方法制备了结构为ITO/SiO2/ZnSe/SiO2/Al的电致发光器件,观察到了传统夹层结构所没有的ZnSe层电致发光.测量了器件的电致发光光谱及总发光强度随着驱动电压及驱动频率的变化关系.讨论了器件的发光机理,认为是初电子经过SiO2层加速,获得较高能量,然后碰撞ZnSe分子,将其价带的电子激发到导带,再跃迁回价带或缺陷能级与空穴复合发光.由于这种发光方式类似于阴极射线发光,只不过电子在固体中而不是真空中加速,所以称之为固态阴极射线发光.这种机理为实现蓝色电致发光提供了新的途径.     

ZnSe为发光层的蓝绿光薄膜电致发光器件的发光性能

采用具有电子加速能力的Si02代替传统夹层结构中的绝缘层,利用电子束蒸发的方法制备了结构为ITO/SiO2/ZnSe/SiO2/Al的电致发光器件,观察到了传统夹层结构所没有的ZnSe层电致发光.测量了器件的电致发光光谱及总发光强度随着驱动电压及驱动频率的变化关系.讨论了器件的发光机理,认为是初电子经过SiO2层加速,获得较高能量,然后碰撞ZnSe分子,将其价带的电子激发到导带,再跃迁回价带或缺陷能级与空穴复合发光.由于这种发光方式类似于阴极射线发光,只不过电子在固体中而不是真空中加速,所以称之为固态阴极射线发光.这种机理为实现蓝色电致发光提供了新的途径.     

一种新结构中ZnSe薄膜电致发光特性研究

用电子束蒸发的方法制备了一种新的ITO／SiO2／ZnSe／SiO2／Al薄膜电致(TFEL)发光器件。在交流电压驱动下,其有2个发光峰,分别位于466nm和560nm。通过研究器件(PL)激发(PLE)谱、光致发光、EL发光以及EL发光强度随驱动电压和频率的变化发现,器件的发光来源于ZnSe的带边发射和自激活发光中心。器件的发光机理与一般的无机电致发光有所不同。这里,SiO2作为电子加速层,ZnSe作为发光层,电子在SiO2层中的高电场作用下被加速到很高的能量,然后直接碰撞激发ZnSe分子使其发光。这种发光现象被称为固态类阴极发光。     

非对称绝缘层无机EL显示器件的研究

非对称绝缘层无机EL显示器件是一种新颖的器件结构。成功制备了一批ZnS：Mn器件，其下介质层为厚100-200nm的SrTiO3（ST）或Ba0．5Sr0．5TiO3（BST）或Ta2O5薄膜，上介质层为厚600～1100nm的Ta2O5或ST／Ta2O5或HfO2／Ta2O5／Al2O3薄膜。发现以ST／Ta2O5为上介质层的器件具有适当的阈值电压、较高的L50和较陡的L—V曲线，以HfO2／Ta2O5／Al2O3为上介质层的器件具有较高的可靠性。     

薄膜EL器件

这是有关用作显示器件的薄膜 EL 器件的发明.近来,碱土类硫硒碲化合物为基质、Ce激活发光层的薄膜 EL 器件,由于它能得到较高亮度的蓝色发光而受到重视。这种薄膜EL 器件,通常是在 SrS 和 SrSe 碱土类硫硒碲化合物(用溅射方法或真空蒸发方法形成)中,把其中一种化合物作为基质,用 Ce 激活的薄膜用来做发光层。以 SrS 或 SrSe 为基质,用 Ce 激活的发光层作为薄膜 EL 器件,能够得到 ZnS 基质发光EL 器件所不可能达到的高亮度蓝色发光。     

MEH-PPV的短波光与传导电流关系

采用MEH-PPV和SiO2复合制成异质结固态阴极射线发光器件,获得了固态阴极射线发光的特征光谱-双峰谱带。在电场较低时为激子发光,符合分子理论;在电场较高时激子已严重离化,属于带-带跃迁,符合能带理论。利用改进的电桥测量出传导电流,并研究了固态阴极射线发光蓝色发光强度同传导电流的关系。在低电压区,发光强度同传导电流关系近似为线性,在高电压区,由于SiO2的二次特性更加突出,发光强度同传导电流关系表现出超线性。     

基于双绝缘层低电压n-型OFET的研制

采用顶接触结构研制了以Ta2O5/PMMA为绝缘层,有机材料PTCDI-C12为有源层的低电压n型有机场效应晶体管.其中Ta2O5薄膜采用阳极氧化方法制备,PMMA薄膜通过溶液旋涂法制备.与基于单一Ta2O5绝缘层的器件相比,双绝缘层器件的电学性能大幅提高.经测试得到器件场效应电子迁移率为0.063 cm2/Vs,开关电流比为1.7×104,阈值电压为2.3 V.     

Nb2O5空穴注入层的引入对OLEDs性能的影响

在有机发光二极管典型的层状结构中,引入磁控溅射制备Nb2O5超薄膜作空穴注入层,制备了结构为ITO/Nb2O5/TPD/Alq3/A1的器件.Nb2O5层的引入,降低了空穴注入势垒,增强了空穴注入,同时有效阻挡了ITo中ln向有机层的扩散,减少了发光猝灭中心的形成,提高了器件的亮度和效率.研究了不同厚度Nb2 O5层对器件光电性能的影响,发现:当引入Nb2O5层厚度为2 nm时,亮度提高了近2倍,效率由3.5 cd/A增加到了7.8 cd/A,较好地改善了器件的性能,并且性能优于含有CuPc常规注入层的器件.     

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.     

用新型ZnS/SrS:Ce多层荧光粉的ACTFEL器件

讨论了用多层 ZnS/SrS:Ce 的 acTFEL器件,用 ZnS 和 SrS:Ce 分9次交替地蒸发堆积构成,在60Hz,50μs 的脉冲激发下,蓝色发光的最高亮度超过10cd/m~2。在全色的 EL—显示器中,蓝色发光的亮度首次达到应用的要求,这种多层的器件在加速老化时是稳定的。     

Low voltage n-type OFET based on double insulators

A top contact n-type organic field-effect transistor with low operating voltage was fabricated by employing Ta2O5/PMMA as the double insulators and PTCDI-Cl2 as the semiconductor active layer. The Ta2O5 layer was prepared by using simple economical anodization technique and the PMMA layer was prepared by using the spin-coating method. Compared with the OFET with single Ta2O5 insulator, the device with double insulators shows obviously better electrical performance. It has a field effect electron mobility of 0.063 cm^2/Vs, an on/off ratio of 1.7 × 10^4 and a threshold voltage of 2.3 V.     

Flexible AM OLED panel driven by bottom-contact OTFTs

Active matrix organic-light-emitting-diode (AM OLED) panels, driven by organic thin-film transistors (OTFT), have been successfully fabricated on a flexible plastic substrate. The pixel circuit consists of two bottom-contact pentacene OTFTs working as switching and driving transistors. The panel has 16 /spl times/ 16 pixels, each of which have an OLED using a phosphorescent material with an emission efficiency of 30 cd/A. A tantalum oxide (Ta/sub 2/O/sub 5/) film with a dielectric constant of 24, prepared by the anodization of Tantalum (Ta), was used as the gate insulator of the OTFTs. The passivation layer on the OTFTs was formed by a layer of silicon dioxide (SiO/sub 2/) and two layers of polyvinyl alcohol. Using OTFTs with a Ta/sub 2/O/sub 5/ gate insulator, the authors have realized a flexible active matrix OLED panel driven with a low voltage of -12 V.     

聚合物电致发光器件中用类金刚石碳膜增强电子注入

用正丁胺作碳源,采用射频辉光等离子系统制备类金刚石碳膜(DLC),沉积在聚合物发光器件中的发光层(MEH-PPV)和铝(Al)阴极间作电子注入层.制备了结构为ITO/MEH-PPV/DLC/Al的不同DLC厚度的器件,测量了器件的I-V特性、亮度及效率,研究了DLC层对器件电子注入性能影响的机制.结果表明:当DLC厚度小于1.0nm时,其器件有较ITO/MEH-PPV/Al高的启动电压和低的发光效率;当DLC厚度在1.0～5.0nm之间时,器件的性能随着DLC厚度增加而变好;当DLC厚度为5.0nm时,器件具有最低的启动电压与最高的发光效率;当DLC厚度继续增加时,器件的性能随着DLC厚度增加而变差.并对ITO/MEH-PPV/DLC/Al和ITO/MEH-PPV/LiF/Al的器件性能进行了比较研究.     

Electron Injection Enhancement by Diamond-Like Carbon Film in Polymer Electroluminescence Devices

用正丁胺作碳源,采用射频辉光等离子系统制备类金刚石碳膜(DLC),沉积在聚合物发光器件中的发光层(MEH-PPV)和铝(Al)阴极间作电子注入层.制备了结构为ITO/MEH-PPV/DLC/Al的不同DLC厚度的器件,测量了器件的I-V特性、亮度及效率,研究了DLC层对器件电子注入性能影响的机制.结果表明:当DLC厚度小于1.0nm时,其器件有较ITO/MEH-PPV/Al高的启动电压和低的发光效率;当DLC厚度在1.0～5.0nm之间时,器件的性能随着DLC厚度增加而变好;当DLC厚度为5.0nm时,器件具有最低的启动电压与最高的发光效率;当DLC厚度继续增加时,器件的性能随着DLC厚度增加而变差.并对ITO/MEH-PPV/DLC/Al和ITO/MEH-PPV/LiF/Al的器件性能进行了比较研究.     

MIM薄膜二极管Ta_2O_5绝缘膜的AFM分析及其I-V特性研究

制备了一种用于有源矩阵液晶显示的Ｔａ－Ｔａ２Ｏ５－Ｔａ 结构ＭＩＭ 薄膜二极管。其中,作为介质层的Ｔａ２Ｏ５ 膜由不同成膜技术得到。采用原子力显微镜（ＡＦＭ）对Ｔａ２Ｏ５ 膜进行了表面形貌分析,并对其ＭＩＭ 二极管的伏安特性进行了测试与比较。结果表明,用溅射／阳极氧化二步法制备的Ｔａ２Ｏ５ 膜作绝缘层的ＭＩＭ 二极管,其Ｉ－Ｖ特性的非线性系数β＝ ２５,远高于阳极氧化法及溅射法所得Ｔａ２Ｏ５ 膜的ＭＩＭ 二极管的非线性系数（β＝ ９和５）,电流通断比（１０５）分别较阳极氧化法及溅射法工艺制备的ＭＩＭ－ＴＦＤ高１和３ 个数量级,且其伏安特性的对称性也较好     

Bicolor Light-Emitting Diode Based on Zinc Oxide Nanorod Arrays and Poly(2-methoxy,5-octoxy)-1,4-phenylenevinylene

The current study reports a novel inorganic/organic light-emitting diode (LED), consisting of zinc oxide (ZnO) nanorod arrays and poly(2-methoxy, 5-octoxy)-1,4-phenylenevinylene (MOPPV). ZnO nanorod arrays passivated using polyacrylamide (PAM) with 70 nm diameter were successfully prepared by a simple polymer-assisted chemical method. Enhancement of the ZnO defect emission is caused by PAM passivation, as observed in photoluminescence spectra. Infrared absorption spectra reveal that PAM is chemically or physically adsorbed on the surfaces of ZnO nanorod arrays. The electroluminescence (EL) spectrum shows bluish light at 406 nm from ZnO transition emission, and light emission with center at 600 nm from exciton emission in MOPPV. The potential EL mechanism is electron transition to zinc vacancy in PAM/ZnO nanorod arrays, and exciton radiation luminescence in MOPPV film. This novel PAM/ZnO-MOPPV device may be helpful to promote development of multicolor LEDs.     

Synthesis of polymers for hole and electron transport materials inorganic electroluminescent devices

Styrene-type polymers having tetraphenylbenzidine (TPD) or tetraphenylphenyldiaminobenzene unit (PDA) and a oxadiazole unit (PBD) on the side chain were prepared as hole and electron transport materials, respectively, of an electroluminescent (EL) device. The device structures employed were [indium-tin-oxide (ITO)/hole transport layer (HTL)/Al] (type I), or [ITO/hole transport layer (HTL)/electron transport layer (ETL)/Al] (type II). Type I devices provided current density higher than 100 mA/cm² but no luminescence was observed. Type II devices emitted luminescence of about 10 cd/m² at the current density of about 170 mA/cm². The emission maximums of these devices were 460 and 530 nm for the device using TPD and PDA, respectively     

Pure and Saturated Red Electroluminescent Polyfluorenes with Dopant/Host System and PLED Efficiency/Color Purity Trade‐Offs

Three kinds of red electroluminescent (EL) polymers based on polyfluorene as blue host and 2,1,3‐benzothiadiazole derivatives with different emission wavelengths as red dopant units on the side chain are designed and synthesized. The influence of the photoluminescence (PL) efficiencies and emission wavelengths of red dopants on the EL efficiencies and color purities of the resulting polyfluorene copolymers of dopant/host system is investigated by adjusting the electron donating ability of the donor units in D‐π‐A‐D typed 2,1,3‐benzothiadiazole derivatives. The devices of these red‐emitting polymers realize remarkable EL efficiency/color purity trade‐offs. The single‐layer devices with the configuration of ITO/PEDOT:PSS/Polymer/Ca/Al show pure red emission at 624 nm with a luminous efficiency of 3.83 cd A^?1 and CIE of (0.63, 0.35) for PFR1, saturated red emission at 636 nm with a luminous efficiency of 2.29 cd A^?1 and CIE of (0.64, 0.33) for PFR2, respectively. By introduction of an additional electron injection layer PF‐EP(Ethanol soluble phosphonate‐functionalized polyfluorene), high performance pure and saturated red emission two‐layer devices (ITO/PEDOT:PSS/Polymer/PF‐EP/LiF/Al) were achieved with maximum luminous efficiencies of 5.50 cd A^?1 and CIE of (0.62, 0.35) for PFR1, 3.10 cd A^?1 and CIE of (0.63, 0.33) for PFR2, respectively, which are the best results for pure and saturated fluorescent red EL polymers reported so far.