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有机发光材料DPVBi的空穴阻挡特性
引用本文:姜文龙,王静,丁桂英,汪津,王立忠,韩强,刘式墉. 有机发光材料DPVBi的空穴阻挡特性[J]. 发光学报, 2006, 27(4): 561-565
作者姓名:姜文龙  王静  丁桂英  汪津  王立忠  韩强  刘式墉
作者单位:吉林师范大学,信息技术学院,吉林,四平,136000;吉林大学,集成光电子学国家重点联合实验室,吉林,长春,130023;吉林师范大学,信息技术学院,吉林,四平,136000;吉林大学,集成光电子学国家重点联合实验室,吉林,长春,130023
基金项目:吉林省科技发展计划(20050523),吉林省教育厅科研计划(吉教科合字[2003]第25号,[2004]第54号),四平科技局计划(四科合字第20030017号)资助项目
摘    要:讨论了有机发光材料4,4′-bis(2,2′-diphenylvinyl)-1,1′-biphenyl(DPVBi),在结构为ITO/N,N′-bis-(1-naphthyl)-N,N′-diphenyl-1,1′-biphenyl-4,4′-diamine(NPB)/DPVBi/tris-(8-hydroxyquinoline)aluminum(Alq3)/LiF/Al的有机电致发光器件中所表现出来的空穴阻挡特性。通过实验可以看到,当NPB的厚度小于DPVBi的厚度时,DPVBi对空穴的阻挡作用和其自身的厚度有关,厚度越大阻挡能力越强。DPVBi的厚度一定(120nm)且不足以将空穴完全限制于DPVBi层内时,其对空穴的阻挡能力,随着NPB厚度(30~60nm)的增加而相对减弱。当NPB的厚度大于DPVBi的厚度时,进入DPVBi层的空穴,随着它们之间厚度差别的增大而增加,从而使器件的光谱半峰全宽加大。这几条规律对于制作基于DPVBi的有机蓝光和有机白光器件具有一定的指导意义。

关 键 词:有机电致发光材料  空穴  空穴阻挡特性
文章编号:1000-7032(2006)04-0561-05
收稿时间:2005-12-20
修稿时间:2006-01-05

Hole-blocking Characteristics of Organic Light Emitting Materials DPVBi
JIANG Wen-long,WANG Jing,DING Gui-ying,WANG Jin,WANG Li-zhong,HAN Qiang,LIU Shi-yong. Hole-blocking Characteristics of Organic Light Emitting Materials DPVBi[J]. Chinese Journal of Luminescence, 2006, 27(4): 561-565
Authors:JIANG Wen-long  WANG Jing  DING Gui-ying  WANG Jin  WANG Li-zhong  HAN Qiang  LIU Shi-yong
Affiliation:1. College of Information Technology, Jilin Normal University, Siping 136000, China;2. State Key Laboratory on Integrated Optoelectronics, Jilin University, Changchun 130023, China
Abstract:The hole-blocking characteristics of organic light emitting materials DPVBi were discussed.The(device) structure included indium tin oxide glass(ITO) substrate/N,N′-bis-(1-naphthyl)-N,N′-diphenyl-1,1′-biphenyl-4,4′diamine(NPB) as hole transparent layer/DPVBi as emitting layer/40 nm tris-8hydroxyquinoline aluminum(Alq3) as electron transport layer/0.5 nm LiF/100 nm aluminum(Al).Organic materials were deposited by vacuum deposition at 1.33×10-4 Pa using resistively heated tan-(talum) and quartz boats.The doping was carried out using the co-evaporation method.The layer thickness of the deposited material was monitored in situ using an oscillating quartz thickness monitor.Finally a LiF buffer(layer) and Al cathode were deposited at a background pressure of 1.33×10-4 Pa onto the organic films.EL spectra and CIE coordination of the devices were measured by PR650 spectra scan spectrometer and the current-voltage-brightness characteristics were simultaneously measured by a Keithley 2400 programmable voltage-current source.All measurements were carried out at room temperature under ambient conditions.The experiment results show that the hole-blocking characteristic is related to the DPVBi thickness and the NPB thickness.While NPB thickness is less than DPVBi thickness,the hole-blocking capacity of DPVBi increases as DPVBi thickness (increases).The hole-blocking capacity of DPVBi decreases as NPB thickness increases when the DPVBi thickness is unchanged(120 nm).While NPB thickness is more than DPVBi thickness,the hole-blocking capacity of DPVBi increases as their thickness difference increases.The hole that through the DPVBi layer into the Alq3 layer increase,causing the full width at half maximum(FWHM) of the emission spectrum is broaden.In the conclusion,when DPVBi was used to fabricate the organic blue-light device in order to ensure the luminance and efficiency of the device,the exciton in DPVBi layer should be limited,the emission of Alq3 should be controlled,the FWHM of emission spectra should be decreased,and the chroma of device will be improved.As far as organic white-light device is concerned,the thickness difference between NPB and DPVBi should be controlled when the total thickness of device is less than 100 nm.The method we adopted enables the emissions of each kind of material to achieve equilibrium and the performance of the organic white-light device can be improved obviously.
Keywords:organic light emitting materials  hole  hole-blocking characteristics  
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