共查询到20条相似文献,搜索用时 125 毫秒
1.
2.
研究了AZO(ZnO∶Al)替代ITO透明导电膜在GaN基LED中的应用,通过脉冲激光沉积和磁控溅射法制作了AZO薄膜,分析了AZO与p型GaN不良的欧姆接触的物理机理,并利用插入ITO薄层来改善接触电阻,实验用ITO 20nm/AZO 500nm的复合导电薄膜做透明导电薄膜,成功得到了波长为525.74nm、亮度为380.88mcd、电压为3.35V的GaN基绿光LED芯片,相当于单一ITO透明导电膜的性能,整个试验工艺中减少了ITO的使用量,降低了LED芯片的制造成本。 相似文献
3.
4.
用于液晶光阀空间光调制器的ITO透明导电膜的研制 总被引:1,自引:0,他引:1
本文介绍了ITO(Indium Tin Oxide)透明导电膜的制备工艺,对影响其光学和电学特性的因素作了分析。并讨论了透明导电的机理,在K9玻璃上制备的ITO透明导电膜,在500~600nm波长范围内,典型的峰值透过率为90%,面电阻为40~50Ω/□。用该技术制备的样品作为透明电极,在液晶光阀空间光调制器中得到了应用。 相似文献
5.
对嵌埋于玻璃基体中的CdS0.1Sc0.9纳米晶体进行了室温电调制透射谱测量,观察到较强的共振和非共振电光响应倚号(10-4~10-3).共振电光响应具有如下特征:同一组分的纳米晶体其倩号的峰位随着尺寸减小向高能方向移动;同一样品谱线形状不随外电场强度而变;信号幅度与外电场强度的平方成线性关系,并且随调制频率的增加而减小;共振电光效应的物理机制是量子受限的Stark效应.非共振电光响应信号呈与波长有关的振荡线形;外电场强度增加,非共振电光响应信号幅度也增加;用介电受限的局域场增强理论解释了非共振电光效应的物理机制. 相似文献
6.
研究了不同厚度ITO膜的大尺寸超薄导电玻璃的翘曲度,ITO膜形成期间基片温度对ITO膜层晶体化程度的影响及不同基片温度下形成的ITO膜层在不同的退火条件下的退火前、后的电阻率和膜压应力.实验发现,ITO膜层的很高的压应力是导致导电膜玻璃翘曲的直接原因;采用室温沉积非晶ITO膜,然后经高温热退火可获得低膜压应力多晶相ITO膜.基于实验结论,提出了一种适合批量生产的低翘曲度ITO膜导电玻璃的制备工艺. 相似文献
7.
采用金属有机化学气相沉积(MOCVD)技术在蓝宝石衬底上制备了GaN基LED外延层,采用磁控溅射法制备了氧化铟锡(ITO)薄膜,ITO薄膜用于制作与p-GaN的欧姆接触.研究了快速热退火温度为550℃,退火时间为200 s时,不同氧气体积流量对ITO薄膜性能及LED芯片光电性能的影响.结果表明:不通氧气时,ITO薄膜的方块电阻和透过率分别为33 Ω/口和93.1%,LED芯片出现电流拥挤效应,其电光转换效率只有33.3%;氧气体积流量为1 cm3/min时,ITO薄膜的方块电阻和透过率分别为70 Ω/口和95.9%,LED芯片的电流扩展不佳,其正向电压较高,电光转换效率为43.8%;氧气体积流量为0.4 cm3/min时,ITO薄膜的方块电阻和透过率分别为58 Ω/口和95.4%,LED芯片的电流扩展最佳,其亮度最高、正向电压最低,电光转换效率较高,为52.9%. 相似文献
8.
ITO薄膜的溶胶-凝胶法制备 总被引:2,自引:0,他引:2
介绍了几种用溶胶 凝胶法制备ITO薄膜的工艺方法 ,用其中一种无机的方法成功制备了ITO透明导电膜。当薄膜厚度为 30 0nm左右时 ,所得ITO薄膜在可见光区域内的平均透过率在 85 %以上 ,电阻率最低可达 0 .1 5Ω·cm。 相似文献
9.
这种2mm 厚电致发光(EL)触摸板用浸涂工艺制成,具有双面氧化铟锡(ITO)透明导电膜,电耗为发光二极管(LED)板的1/3,作为 LCD 背光源时,功耗小于发光二极管的1/10。ITO 膜的开发者松下电器实业公司应用他们的新式膜和 Showa Shell Sekiyu 制造的EL 板,设计了这种新型的触摸板。双面导电膜用无机铟化合物、有机锡化合物和有机溶剂 相似文献
10.
11.
The effects of contact electrode size on the photo-voltaic characteristics of polycrystalline-Si p-i-n solar cells have been studied,with respect to a unit-cell pitch size of 1μm width.For the non-transparent Al contact electrode with a contact width of 0.05-0.2μm,the short-circuit current is obviously reduced with increasing contact width,due to a larger area of optical reflection by the electrode.On the other hand,even when using a transparent ITO(indium-tin-oxide) electrode,a larger width of contact electrode may also cause a smaller short-circuit current, due to a larger area of optical absorption by the electrode.However,for this ITO electrode,the contact electrode of 0.05μm width causes a smaller short-circuit current than that of 0.1μm width,primarily ascribed to a smaller area for collecting carrier and a larger contact resistance.As a result,while using the ITO contact electrode to enhance the conversion efficiency of the solar cell,a proper width of contact electrode should be employed to optimize the photo-voltaic characteristics. 相似文献
12.
S. Khodabakhsh D. Poplavskyy S. Heutz J. Nelson D.D.C. Bradley H. Murata T.S. Jones 《Advanced functional materials》2004,14(12):1205-1210
Surface modification of indium‐tin‐oxide (ITO)‐coated substrates through the use of self‐assembled monolayers (SAMs) of molecules with permanent dipole moments has been used to control the ITO work function and device performance in polymer light‐emitting diodes based on a polyfluorene hole transporting copolymer. Measured current–voltage characteristics of the devices reveal greatly increased hole injection currents from the SAM‐altered electrodes with higher work function, in agreement with an expected reduction in the barrier for hole injection. In particular, it is shown that the SAM‐modified electrode with the highest work function provides an ohmic contact for hole injection into the studied polymer. Injection from the widely used poly(2,3‐ethylenedioxythiophene)/polystyrenesulphonic acid (PEDOT:PSS)‐coated ITO anode system, is less efficient compared with some of the studied SAM‐coated ITO anodes despite the significantly higher work function measured by a Kelvin probe. This apparently anomalous situation is attributed to the inhomogenities in the injection processes that occur over the area of the device when the PEDOT:PSS‐coated ITO electrode is used. 相似文献
13.
14.
15.
《Display Technology, Journal of》2009,5(6):188-191
16.
Hongfei Liu Alin Hou Hongbo Zhang Daming Zhang Maobin Yi 《Microelectronics Reliability》2007,47(1):82-87
This paper simulates the electric potential distribution and the electro-optic (EO) signal amplitude in a longitudinal poled EO polymer external probe tip on the electric signal transmission lines under test. The influence of the circuit layout on the EO probing is discussed. A novel probing configuration with a poled polymer EO probe tip is built and demonstrated for the first time, by which the signal voltage level corresponding to the EO signal can be calibrated. Using the new probe tip, we examine the influence of the variations of the linewidth and the spacing between neighboring lines on the EO signal. The results indicate that when the vertical distance between the tested point on the lines and the reference electrode is not larger than that between the tested point and its neighboring conductor, the disturbance from circuit layout can be avoided so that the voltage calibration of EO signal can be carried out. 相似文献
17.
Achieving Above 60% External Quantum Efficiency in Organic Light‐Emitting Devices Using ITO‐Free Low‐Index Transparent Electrode and Emitters with Preferential Horizontal Emitting Dipoles
下载免费PDF全文
![点击此处可从《Advanced functional materials》网站下载免费的PDF全文](/ch/ext_images/free.gif)
Chun‐Yang Lu Min Jiao Wei‐Kai Lee Chien‐Yu Chen Wei‐Lung Tsai Chun‐Yu Lin Chung‐Chih Wu 《Advanced functional materials》2016,26(19):3250-3258
Comprehensive theoretical and experimental studies are reported on organic light‐emitting devices (OLEDs) adopting either the conventional high‐index indium tin oxide (ITO) electrode or the low‐index conducting polymer electrode, either isotropic emitters or emitters having preferentially horizontal emitting dipoles, and different layer structures. Intriguingly, with the use of low‐index electrode in the device, in addition to the known suppression of waveguided modes, the surface plasmon modes can also be effectively suppressed with larger emitter‐to‐metal distances yet with better immunity to accompanied increase of the competing waveguided modes (induced by thicker organic layers) as in the ITO device. As a result, overall coupling efficiencies of OLED internal radiation into substrates can be significantly enhanced over those with ITO electrodes. Through effective extraction of radiation within substrates, green phosphorescent OLEDs adopting both the low‐index ITO‐free electrode and the preferentially horizontal dipole emitter (with a horizontal dipole ratio of 76%) achieve a high external quantum efficiency (EQE) of up to ≈64%. The simulation also predicts that very high EQEs of ≥80% are possible with highly horizontal dipole emitters for all red/green/blue/white OLEDs, clearly revealing the potential of combining low‐index transparent electrodes and horizontal dipole emitters for high‐efficiency OLEDs. 相似文献
18.
为了提高石英晶体微天平(QCM)的检测灵敏度,提出了一种具有氧化铟锡(ITO)电极结构的QCM。利用有限元分析软件在QCM芯片电极区采用密度等效法实现计算量的简化,在通过电极尺寸优化得到具有理想能陷效应的QCM的基础上,采用控制磁控溅射的气体压强、工作电压、电流等方法,得到具有导电性好,平滑度高,透光性优良的ITO电极。经振荡频率测试及质量灵敏度分析计算表明,ITO电极的QCM频率稳定性良好(频率变化仅3 Hz),质量灵敏度是金电极QCM的1.5倍。 相似文献
19.
20.
基于本实验室的实验条件,采用射频磁控溅射、等离子干法刻蚀等技术成功制备出具有ZnO∶Ga(GZO)透明电极的LED芯片。实验研究了相同工艺条件制备的ITO透明电极LED芯片和GZO透明电极LED芯片,对比实验结果表明GZO薄膜沉积工艺简单,其器件性能与ITO电极LED相当。相同条件下制备的GZO薄膜可见光波段透过率约90%,而ITO仅为75%。实验室制备的LED器件均具有较高的阈值电压,一方面p-GaN与ZnO的禁带宽度相差4.13 eV,接触势垒大,另一方面器件制备过程中的等离子体损伤薄膜表面和器件性能。 相似文献