一种新型插层结构的有机电致发光器件

报道了一种新型插层结构的有机电致发光器件(OLED),LiF(1 nm)/Al(5 nm)插层作为半反射镜,与LiF(1 nm)/Al(100 nm)作为全反射镜面的阴极构成平面Fabry-Perot(F-P)型微腔,所用发光层材料为Zn(salen),器件的结构为:ITO/CuPc/NPD/Zn(salen)/Liq/LiF/Al/CuPc/NPD/ Zn(salen)/Liq/LiF/Al,其最大发光亮度和电流效率分别达674 cd/m2 和 2.61 cd/A,半峰宽(FWHM)为48 nm.与传统结构器件相比,色纯度、发光亮度和发光效率等性能指标均得到了优化.     

微腔结构对红光磷光OLED的性能的影响研究

使用新型红光磷光材料R-4B作为微腔有机电致发光显示器(OLED)的发光层,高反射Al阴极和半透半反Al阳极为微腔的两端反射镜。制备的器件结构为Al(10nm)/MoOx(Ynm)/NPB(40nm)/TCTA(10nm)/CBP:R-4B(4%)(30nm)/BCP(10nm)/AlQ(40nm)/LiF(1nm)/Al(100nm)。讨论了腔长的变化对器件性能的影响。结果表明,微腔结构可以使光谱窄化,随着MoOx厚度Y的增加,其峰值波长由600nm增至668nm。当MoOx厚度为40nm时,其发光强度最大,峰值波长为608nm,半高宽(FWHM)为50nm,器件的最大亮度为35 300cd/cm2,最大效率可达23.5cd/A,得到了性能较好的红色磷光OLED。     

插入层TmP_yPb对白色有机电致发光二极管色纯度的影响

基于三原色白光器件ITO/NPB/TCTA/Ir(MDQ)2(acac)∶TCTA/TCTA/FIrpic∶TmPyPb/Ir(ppy)3∶TmPyPb/TmPyPb/LiF/Al,通过在其绿色与蓝色发光层之间插入不同厚度的TmPyPb,研究了该插入层的厚度对器件色纯度的影响。研究表明,插入层厚度的改变能够影响能量转移及调节激子的分布,当插入层厚度为4nm时,器件色坐标为(0.33,0.36),最大发光效率达11.58cd/A。     

2-TNATA对蓝与黄二基色分离的堆叠式白色有机发光器件性能的影响(英文)

研究了2-TNATA厚度对蓝与黄二基色分离的堆叠式白色有机发光器件性能的影响。器件结构为:2-TNATA(xnm)/NPB(25nm)/ADN(30nm)∶TBPE(2%)∶DCJTB(1%)/Alq3(20nm)/LiF(1nm)/Al(100nm)。根据实验结果,2-TNATA的厚度对载流子的注入、色稳定性、热稳定性影响明显。发光器件的颜色可以通过改变加入的2-TNATA层的厚度来改变。这种器件使用2-TNATA作为空穴注入层显示出了色纯度高的白光发射,CIE色坐标x=0.3197,y=0.3496,亮度能够达到12230cd/m2。     

NPB厚度对堆叠式白光OLED性能的影响

主要研究了NPB厚度对堆叠式白色有机电致发光器件性能的影响。实验制备了四组结构为ITO/2-TNATA(15 nm)/NPB(Tnm)/ADN(30 nm):TBPe(2%):DCJTB(1%)/Alq3(20 nm)/LiF(1 nm)/Al(100 nm)(其中T分别为15,30,35和40 nm)的OLED器件,比较了不同厚度情况下OLED器件的电致发光特性,结果表明:改变NPB(4,4-N,N-bis-N-1-naphthy1-N-pheny1-amino-bipheny1)的厚度能够明显提高器件的发光亮度和发光效率,并调节载流子复合区域的位置,有效提高载流子的注入效果。同时发光器件的颜色也可通过调节NPB层的厚度来改变,这种器件使用NPB作为空穴传输层显示出了色纯度高、亮度好、效率较高的白光发射,其具有CIE色坐标(x=0.301 6,y=0.338 5),最高亮度和最大发光效率分别达到14 020 cd/m2与2.94 lm/W。     

双主体掺杂红色有机电致发光显示器件的研究

利用三源共蒸发技术制作了双主体掺杂红色有机电致发光显示器件,研究了不同掺杂比例下,Alq3∶Rubrene∶DCJTB双主体掺杂系统的红色OLED器件,器件结构为ITO/HIL/NPB/Alq3∶Rubrene∶DCJTB/Alq3/LiF/Al,其中发光层Alq3∶Rubren∶DCJTB是三掺杂发光结构体系。综合研究分析了Alq3与Rubrene的掺杂比例和发光效率、色纯度之间的关系,当Rubrene的掺杂比例达到60%时,器件达到最佳效果;电压9V时,该器件发光亮度达到3580cd/m2,发光效率达到4.58cd/A,功率效率也达到1.60lm/W,相应的色坐标为(0.65,0.35)。     

基于Alq3光耦合层的新型顶发射蓝光有机电致发光器件

研制了一种结构为Ag/Glass/ITO/TAPC/mCP/mCP∶Firpic/TPBi/LiF/Al/Ag/Alq₃的顶发射有机电致发光器件,通过在ITO玻璃衬底背面生长一层Ag反射膜,使器件发出的蓝光被反射膜反射到顶电极出射。利用顶电极表面的Alq₃光耦合层有效地提升了金属复合阴极的透射率,降低了器件的微腔效应。实验结果表明,当光耦合层厚度为30nm时,获得了最大电流效率和最大亮度分别为8.91cd/A和5758cd/m²的蓝光顶发射有机电致发光器件(TEOLED);同时,在10V电压下,其色坐标为(0.157,0.320),当亮度从1cd/m²变化到5000cd/m²时,其色坐标仅漂移(0.002,0.010),表现出良好的色稳定性。     

微腔结构顶发射有机白光器件

结合微腔效应,通过调节不同发光层的厚度制作了顶发射有机白光器件.器件结构为Si/Ag/Ag2O/m-MTDATA/NPB/DPVBi/DCJTB:Alq3/Alq3/LiF/Al/Ag,其中DPVBi,DCJTB与Alq3的掺杂层分别作为蓝光和红光发光层,在选定490 nm的谐振波长时,通过调节DPVBi和掺杂层的厚度来实现对器件发光色度的调节.当DPVBi厚度为1 nm,电压为9 V时,器件的色坐标为(0.33,0.34),非常接近白光等能点.此项工作为利用微腔效应制作高效率高亮度顶发射白光器件奠定了基础.     

基于DSA-ph的高效率超薄层蓝色有机电致发光器件

讨论了基于蓝色荧光染料DSA-ph作为发光层的蓝色有机电致发光器件,器件结构为：ITO/2T-NATA/NPBX/DSA-ph（xnm）/TAZ/Bphen/LiF/Al。通过改变DSA-ph的超薄层厚度,相应器件的性能指标也有所不同。研究表明,在超薄层厚度为0.5nm,驱动电压为4V时,器件的最大发光效率为6.57cd/A;在超薄层厚度为0.3nm时,驱动电压为10V时,器件的最大亮度为5 122cd/m^2。器件的色坐标在（0.17,0.36）附近,属于蓝光发射。     

基于ADN:TBPe发光层的蓝光OLED器件

全色显示是有机电致发光显示(OLED)器件发展的目标,而高性能蓝色发光器件,也是目前有机电致发光显示研究的热点。以NPB和Alq3分别作为空穴传输层和电子传输层,制作了结构为ITO/CuPc(150nm)/NPB(500nm)/ADN(300nm)∶TBPe(30nm)/Alq3(350nm)/RbF(20nm)/Al(1000nm)的蓝光OLED器件,发光亮度达8600cd/m2,发光效率达2.669cd/A,色坐标(X=0.1315,Y=0.1809)。研究发现ADN∶TBPe发光层体系的引入大大改善了蓝光器件的发光效率和性能。     

Tricolor microcavity OLEDs based on P-nc-Si:H films as the complex anodes

A P+-nc-Si:H film (boron-doped nc-Si:H thin film) was used as a complex anode of an OLED. As an ideal candidate for the composite anode, the P+-nc-Si:H thin film has a good conductivity with a high work function (～5.7 eV) and outstanding optical properties of high reflectivity, transmission, and a very low absorption. As a result, the combination of the relatively high reflectivity of a P+-nc-Si:H film/ITO complex anode with the very high reflectivity of an Al cathode could form a micro-cavity structure with a certain Q to improve the efficiency of the OLED fabricated on it. An RGB pixel generated by microcavity OLEDs is beneficial for both the reduction of the light loss and the improvement of the color purity and the efficiency. The small molecule Alq would be useful for the emitting light layer (EML) of the MOLED, and the P+-nc-Si film would be used as a complex anode of the MOLED, whose configuration can be constructed as Glass/LTO/P+-nc-Si:H/ITO/MoO3/NPB/Alq/LiF/Al. By adjusting the thickness of the organic layer NPB/Alq, the optical length of the microcavity and the REB colors of the device can be obtained. The peak wavelengths of an OLED are located at 486, 550, and 608 nm, respectively.The CIE coordinates are (0.21,0.45), (0.33,0.63), and (0.54,0.54), and the full widths at half maximum (FWHM)are 35, 32, and 39 nm for red, green, and blue, respectively.     

基于纳米硅薄膜复合阳极的微腔调色法的研究

A P^＋-nc-Si：H film（boron-doped nc-Si：H thin film） was used as a complex anode of an OLED.As an ideal candidate for the composite anode,the P^＋-nc-Si：H thin film has a good conductivity with a high work function（- 5.7 eV） and outstanding optical properties of high reflectivity,transmission,and a very low absorption.As a result,the combination of the relatively high reflectivity of a P^＋-nc-Si：H film/ITO complex anode with the very high reflectivity of an Al cathode could form a micro-cavity structure with a certain Q to improve the efficiency of the OLED fabricated on it.An RGB pixel generated by microcavity OLEDs is beneficial for both the reduction of the light loss and the improvement of the color purity and the efficiency.The small molecule Alq would be useful for the emitting light layer（EML） of the MOLED,and the P^＋-nc-Si film would be used as a complex anode of the MOLED,whose configuration can be constructed as Glass/LTO/P^＋-nc-Si：H/ITO/MoO3/NPB/Alq/LiF/Al.By adjusting the thickness of the organic layer NPB/Alq,the optical length of the microcavity and the REB colors of the device can be obtained.The peak wavelengths of an OLED are located at 486,550,and 608 nm,respectively.The CIE coordinates are（0.21,0.45）,（0.33,0.63）,and（0.54,0.54）,and the full widths at half maximum（FWHM） are 35,32,and 39 nm for red,green,and blue,respectively.     

光输出增强型微腔OLED器件研究

文章利用特制的玻璃作为OLED基板,一面为平整光滑的平面,另一面为具有规则凹凸形貌的粗化面。采用光输出增强型微腔OLED结构,器件结构为:玻璃基板(光面)/Al(15nm)/MoO3(40nm)/NPB(30nm)/Alq3(30nm):C545T(3%)/Alq3(20nm)/LiF(1nm)/Al(150nm),研究了器件的电流密度、亮度、发光效率、光致发光光谱等特性。结果表明,这种结构的器件相比于传统微腔型器件,相同电压下亮度约增加了40%,发光效率约提高了15%,具有更强的光萃取能力。     

高饱和度蓝色磷光有机发光器件

使用典型天蓝色磷光材料FIrpic作为磷光金属微腔有机发光器件（OLED）的发光层,以高反射的Al膜作为阴极顶电极和半透明的Al膜作为阳极底电极,采用空穴和电子注入层MoO3和LiF,制备了结构glass／Al（15nm）／MoO3（znm）／NPD（40nm）／mCP：Flrpic（30Ftm,7％）／BCP（20n...     

New insert layer structure OLEDs

An insert layer structure organic electroluminescent device（OLED） based on a new luminescent material （Zn（salen）） is fabricated. The configuration of the device is ITO/CuPc/NPD/Zn（salen）/Liq/LiF/A1/CuPc/NPD/Zn（salen）/Liq/LiF/A1. Effective insert electrode layers comprising LiF（1nm）/Al（5 nm） are used as a single semitransparent mirror, and bilayer cathode LiF（1 nm）/A1（100 nm） is used as a reflecting mirror. The two mirrors form a Fabry-Perot microcavity and two emissive units. The maximum brightness and luminous efficiency reach 674 cd/m^2 and 2.652 cd/A, respectively, which are 2.1 and 3.7 times higher than the conventional device, respectively. The superior brightness and luminous efficiency over conventional single-unit devices are attributed to microcavity effect.     

基于MIC多晶硅薄膜阳极的微腔有机发光器件

通过对溶液法金属诱导晶化多晶硅薄膜制备工艺的优化,制备出性能良好的P型掺杂多晶硅薄膜。厚度为50nm的MICP+-Poly-Si薄膜的方块电阻可降低至400Ω左右,其光学特性表现为在红光区域具有比较高的反射率和很小的吸收率,因此用它替代ITO用作红光OLED的阳极材料。由于此薄膜对可见光比较高的反射率和阴极铝对可见光的高反射性,使之形成了一定Q值的微腔效应。结果显示该器件的最大流明效率为5.88cd/A,比用ITO作阳极制备的OLED提高了57%。进一步优化器件结构,调整发光层在腔中的最佳位置,可以大大增强发光强度,从而可以实现发光强度高、单色性好的红色微腔有机电致发光显示器件。     

Suppression of the viewing angle dependence by introduction of nanoporous diffuser film on blue OLEDs with strong microcavity effect

A nanoporous polymer film composed of cellulose acetate butyrate was prepared, which showed an optical haze property of approximately 40%. This film was applied as a diffuser film to improve the viewing angle dependence of microcavity structured organic light emitting diodes (OLEDs). We prepared this film by simply using a spin-coating process with a continuous supply of water mist from a humidifier. Air voids or pores with diameters ranging from 300 nm to 500 nm were found inside the polymer film, to produce three-dimensional (3D) nanoporous polymer films with random distribution. We applied this film to a blue fluorescent OLED device with strong microcavity effect. The film did not affect the total external quantum efficiency (EQE) observed using an integrating sphere. However, the current efficiency collected from the normal direction was reduced by 25%, which means that the film spread out or scattered the light emitted from the OLED device. As a result, we obtained blue microcavity OLEDs with efficiently reduced viewing angle dependency.     

蓝绿色磷光OLED的制备及发光性能研究

以mCP为主体发光材料,蓝绿色磷光染料BGIr1作 为掺杂剂,制备了6种不同BGIr1掺杂量的蓝绿色磷光有机电致发光器件(OLED),研究了不 同掺杂量对蓝绿色磷光OLED器件发光特性的影 响。制得器件的结构为ITO/MoO₃(20nm)/NPB(40nm)/mCP:BGIr1(x%,30nm)/BCP(10nm)/Alq₃(20 nm)/LiF/Al(100nm),其中x%为发光层中磷光染料BGIr1的掺杂量(质量分数)。结果表明,BGIr1掺杂量 为18%时,获得器件的发光性能最佳。18% BGIr 1掺杂器件在488nm和 512nm处获得两个主发射峰,当电 流密度为26.5mA/cm²时,获得最大发光效率为6.2cd/A;在15V驱动电压下,获得最大亮度为6970cd/cm², CIE坐标为(0.17,0.31)。这说明,BGI r1掺杂改善了器件的发光亮度和色纯度,提高了器件的发光效率。     

蓝光OLED的掺杂研究

采用蓝色发光材料ADN为主体发光材料、BAlq3为掺杂材料,通过改变BAlq3的掺杂浓度制备了结构为ITO/NPB/ADN:BAlq3/Alq3/Mg:Ag的一系列蓝光有机发光器件(OLED).研究了器件各有机层之间的能级匹配和BAlq3的掺杂浓度对载流子注入、传输、复合以及发光色纯度的影响.实验结果表明,空穴阻挡材料BAlq3的掺入显著影响OLED的电流密度、发光亮度、发光效率和发光光谱,当BAlq3的掺杂浓度为25%时,OLED的发光效率为1.0 lm/W,发光光谱的峰值为440 nm,色纯度为(0.18,0.15),未封装器件的半衰期为950小时,器件同时满足了高效率和高色纯度的要求.     

基于混合配体Znq(DBM)的单色和白色OLED

以8-羟基喹啉(q)和1,3-二苯基-1,3-丙二酮定向合成了有机小分子配合物Znq(DBM),将其作为发光层制备了单色有机电致发光器件(OLED)。在结构为ITO/m-MTDATA(5nm)/NPB(40nm)/Znq(DBM)(60nm)/LiF(0.5nm)/Al(100nm)的器件中,启亮电压为5V,最大亮度达到4 575cd/m2。同时又在器件中引入间隔层BCP,研究其不同厚度对OLED性能的影响。在结构为ITO/m-MTDATA(5nm)/NPB(40nm)/BCP(x nm)/Znq(DBM)(60nm)/LiF(0.5nm)/Al(100nm)的器件中,当BCP层厚为0nm时,发光颜色为黄绿色;当BCP层厚为1nm时,发光颜色为白色,色坐标为(0.29,0.33),最大亮度为2 231cd/m2;当BCP层厚为5nm时,发光颜色为蓝色。根据器件结构和性能,讨论了其内部机理。