基于N-BDAVBi的高效率双发光层蓝色OLED

采用蓝色有机荧光染料N-BDAVBi作为客体发光材 料,将其分别掺入主体材料ADN和DPVBi中形成双发光层,制备了结构为ITO/m-MTDATA(40nm)/NPB(10nm)/ADN:N-BDAVBi(15nm)/DPVBi:N-BDAVBi(15nm)/TPBi(30nm)/LiF(0.6nm)/Al的高效率蓝色有机荧光器件(OLED)。器件的最大电流效 率为8.13cd/A,对应色坐标为(0.178,0.302) ,电流密度为18.81mA/cm²,分别是ADN:N-BDAVBi和DPVBi: N-BDAVBi作为发光层的单发光层结构器件的2.4和1.8倍。器件性能 提高主要源于双发光层结构减弱了 载流子在界面处的积累,扩大了激子产生区域以及主体与客体之间有效的能量 转移。当驱动 电压为14V时,双发光层器件的最大亮度为20620cd/m²。     

白光有机电致发光器件发光稳定性研究

基于红绿/蓝双发光层,制作了结构为ITO/MoO ₃(10nm)/NPB(40nm)/TCTA(10nm)/CBP:R-4B(2%):GIR1(14%,X nm)/mCP:Firpic(8%,Y nm/BCP(10nm)/Alq₃(40nm)/LiF(1nm)/Al( 100nm)的白色全磷光有机电致发光器件(OLED),通过 调节红绿发光层的厚度X与蓝光发光层的厚度Y,研究了不同发光层厚度器件发 光性能的影响。研究发现:当X 为23nm、Y为7nm时,器件的光效和色坐标都具有 很高的稳定性,在电压分别为5、 10和15V时,色坐标分别为(0.33,0.37)、(0.33,0. 37)和(0.34,0.38);在电压为 5V时,电流密度为0.674mA,亮度为158.7cd ,最大电流效率为26.87cd/A;利用电子阻 挡材料TCTA和空穴阻挡材料BCP能够显著提高载流子的复合效率。分析认为:发光层顺序 为红绿/蓝时,更有利于蓝光的出射,从而使白光的色坐标更稳定。     

发光性能稳定的磷光与荧光复合型白光OLED

使用荧光染料TBPe和Ir(ppy)_2acac 、R-4B两种光染料,采用蓝/红绿双发光层的结构,并结合TPBi对空穴的有效限制作用 ,制备了结构为ITO/MoO₃(X nm)/ADN:(2%)TBPe(30 nm)/CBP:Ir(ppy)_2acac(14%):R-4B(2%)(5nm)/TPBi(10 nm)/Alq₃(30nm)/LiF(1nm )/Al(100nm)的磷光与荧光复合的白光OLED,其中,MoO₃的厚 分别为0、15、20、30和40nm,通过改变MoO₃的厚度调控载流子的注入能力,使用空穴阻挡层提高光效; 通过测量其电压、电流、亮度、色坐标和电致发光(EL)光谱等参数,研究不同厚度的MoO ₃对器件发光性能的影响。结果表明,在MoO₃厚为20nm的情况下,器件的效率滚降 最为平缓。在电压分别 为8、9、10、11、12和13V时,器件的色坐标分别为 (0.31,0.33)、(0.30,0.33)、(0.29,0.33)、(0.29,0.33)、(0.29,0.33)和(0.29, 0.33),具有较高的稳定性,原因为采用 蓝/红绿双发光层结构更有利于蓝光的 出射,且使用ADN主体材料掺杂蓝色荧光染料TBPe作为蓝光发光层降低三重态-三重态 湮灭几率。 研究还发现,在电压为11V、器件的亮度为9744cd/m²和电流密度为11.50mA/cm²时,最大器件的电流效率为 7.0cd/A。     

基于DOPPP的高效白光OLED器件

采用真空热蒸镀的方法,以荧光染料1-(2,5-d imethoxy-4-(1-pyrenyl)-phenyl)pyrene (DOPPP)为蓝发光 层,5,6,11,2-Tetraphenylnaphthacene (Rubrene)为黄发光层,制备了结构为ITO/m-M TDATA(10nm)/NPB(30nm)/ Rubrene (0.2nm)/ DOPPP (x nm)/TAZ(10nm)/Alq₃(30nm)/LiF(0.5nm)/Al的双发光层的高效白色有机电 致发光器件(OLED)。通过调整DOPPP层的厚度,研究器件的发光性能。当DOPPP层厚小 于25nm时,器件以 黄光发射为主;当DOPPP层厚为25nm时器件的性能最佳,在电流密度为209.18mA/cm²时,获得最 大亮度为9232cd/m²,在电流密度为103.712mA/cm²时获得最大电流效率4.68cd/A, 并随着驱动电压 的升高,器件的色坐标从(0.366,0.365)变化到(0.384,0.399),都在白光的范围之内;当DOPPP层厚度超过25nm时,器件的效率和亮度 都开始下降。     

高效率绿色磷光有机电致发光器件

采用真空蒸镀的方法,在真空度为5.0×10－4 Pa条件下,分别以传统的材料CBP、TCTA为主体材料,绿色磷光染 色材料(Ir(ppy)₃)为客体材料,制备了相应的有机电致发光 器件,研究发现采用CBP做主体材料的器件比采用TCTA做主体材料的器件能量传递更充 分。之后制备了结构为ITO/NPB(y_1nm)/ CBP:Ir(ppy)₃(x%,y nm)/TPBi(y_2nm)/LiF(0.5nm)/Al 的有机电致发光器件,进一步探究了器件磷光染色材料的掺杂比、器件总厚度对器件性能的 影响。实验结果表明,以CBP为掺杂主体材料,y=20nm,y₂=40nm,x%=8%,当y₁=65nm, 器件亮度达到最高,为67760cd/m²。当y₁=40nm时 ,器件功率效率最高,为41.2lm/W。与此同时,OLED器件的色坐标 均为(0.30,0.61)。     

加入电子阻挡层的黄色磷光有机电致发光器件

使用绿色磷光材料GIr1和红色磷光材料R-4B作 为掺杂剂,制备了一种黄色磷光有机电致发光 器件(OLED),其结构为ITO/MoO₃(60nm)/NPB(40nm)/TCTA(x nm,x＝0、5、10和15)/CPB:GIr1:R -4B(30nm,14%,2%) /BCP(10nm) /Alq₃(40nm)/LiF(1nm)/Al( 100nm)。其中x＝0,5,10,5nm。通过在发光层与空穴传输层之间增 加电子阻挡层TCTA,使器件的效率得到提高。当TCTA厚为10nm时, 起亮电压为4V左右,器 件的最大发光效率为20.2cd/A,最高亮度可以达到21840cd/m²,器件的色坐标 为(0.42,0.53)。器件的EL主峰位于524nm 和604nm。并且当电流 密度为2.49mA/cm²时,10nm厚的TCTA 电子阻挡层的器件发光效率是不加入TCTA的器件发光效率的2倍。发光效率的提高是由于电 子阻挡层的加入限制了空穴传输层NPB的发光,从而使更多的激子在发光层中复合。     

间隔层提高有机电致发光器件的性能

使用不同的有机材料作为间隔层,制备了基于CB P材料的一系列红绿双发光层有机 电致发光器件(OLED),其结构为ITO/MoO₃(50nm)/NPB(40nm)/TCTA(10 nm)/CBP:R-4B(20nm,2%)/ 间隔层(3nm)/CBP:GIr1(30nm,14%)/BCP(10 nm)/Alq₃(20nm)/LiF(1nm)/Al(100nm),其中间隔 层材料使用BCP、TPBi和TCTA。实验比较了加入不同间隔层后OLED的发光特性,结果显 示,对发光面积为0.8cm²的器件,当器件加入间隔层后,电流效 率和亮度有很大提高,用 TCTA作间隔层时得到器件的最大效率为39.98cd/A,最大亮度为29790cd/m²;并且使用间隔 层后OLED发光性能稳定,电致发光(EL)光谱和色坐标不随驱动电压的变化而产生变化。     

高效率双发光层结构白色荧光有机电致发光器件

通过将橙色荧光染料Rubrene和蓝色荧光染料BCzVBi分别掺入NPB和DPVBi中作为发光层,制备了结构为ITO/m-MTDATA(30nm)/NPB(20nm)/NPB∶0.5wt% Rubrene(10nm)/DPVBi∶5wt% BCzVBi(15nm)/Bphen(25nm)/LiF(0.6nm)/Al的双发光层结构白色有机荧光电致发光器件。器件发光主要是Rubrene直接俘获载流子和主体材料DPVBi到客体BCzVBi的能量传递两种发光机制竞争的结果。在低压下Rubrene俘获载流子发光占主导地位,导致器件的橙光相对较强,随电压升高主客体能量传递增强,使蓝光相对强度增强。器件最大电流效率为6.5cd/A,最大亮度为16 140cd/m2。亮度从1 000cd/m2增加到10 000cd/m2,器件的发光色坐标从(0.33,0.37)变化到(0.30,0.32),始终处于白光区。     

具有不同掺杂层厚度的荧光与磷光材料相结合的高效白色有机发光器件

实验制作一种多层白色有机发光器件(WOLED)。将 绿光磷光材料和红光磷光材料 Ir(piq)₂(acac)共掺到母体BPhen中作为绿光和红光发光层;荧光材料DPVBi作为蓝光发 光层,通过改变掺杂层的厚度,得到了高效率的白色WOLED。器件的最大电流效 率可达4.55cd/ A,14 V时亮度达8489cd/m² ;当电压从4V变化到12 V时,色坐标从(0.52,0.34)变化到(0.34, 0.26),基本处于白光区。此器件的 特点,在于其性能可以通过简单地调整掺杂层的厚度来控制。     

磷光与荧光相结合的多层白色有机发光器件

采用真空热蒸镀的方法制备了磷光与荧光相结合的 多层白色有机电致发光器件(OLED)。将绿 光磷光掺杂染料掺杂到母体CBP中作为绿光发光层;荧光材料 DCM2以亚单层的方式插入Alq₃中作为红光发光层;DPVBi为蓝光发光层。器件的结构为ITO /NPB(40nm)/DPVBi(d nm)/CBP:Ir(ppy)₃₈%(5nm)/ Alq₃(5nm)/DCM2(0.05nm)/Alq₃(45nm)/LiF(1nm)/AI(200nm)。实验中通过改变蓝光发 光层的厚度,得到了高效率的 白光OLED,器件的最大电流效率可达6.75cd/A,最大功率效率达2.67lm/W,最大亮度 达30440cd/m²。此外,当电压从4V变化到14V时色坐标从(0.59,0.39)变化到(0.35,0.38), 基本处于白光区。本文器件的特点在于其性能可以通过简单调整DPVBi的厚度,避免 了使用多掺杂层工艺的复杂性。     

Molecular Engineering of Blue Fluorescent Molecules Based on Silicon End‐Capped Diphenylaminofluorene Derivatives for Efficient Organic Light‐Emitting Materials

Blue fluorescent materials based on silicone end‐capped 2‐diphenylaminofluorene derivatives are synthesized and characterized. These materials are doped into a 2‐methyl‐9,10‐di‐[2‐naphthyl]anthracene host as blue dopant materials in the emitting layer of organic light‐emitting diode devices bearing a structure of ITO/DNTPD (60 nm)/NPB (30 nm)/emitting layer (30 nm)/Alq₃ (20 nm)/LiF (1.0 nm)/Al (200 nm). All devices exhibit highly efficient blue electroluminescence with high external quantum efficiencies (3.47%–7.34% at 20 mA cm^?2). The best luminous efficiency of 11.2 cd A^?1 and highest quantum efficiency of 7.34% at 20 mA cm^?2 are obtained in a device with CIE coordinates (0.15, 0.25). A deep‐blue OLED with CIE coordinates (0.15, 0.14) exhibits a luminous efficiency of 3.70 cd A^?1 and quantum efficiency of 3.47% at 20 mA cm^?2.     

Stable,Glassy, and Versatile Binaphthalene Derivatives Capable of Efficient Hole Transport,Hosting, and Deep‐Blue Light Emission

Organic light‐emitting diodes (OLEDs) have great potential applications in display and solid‐state lighting. Stability, cost, and blue emission are key issues governing the future of OLEDs. The synthesis and photoelectronics of a series of three kinds of binaphthyl (BN) derivatives are reported. BN_1–3 are “melting‐point‐less” and highly stable materials, forming very good, amorphous, glass‐like films. They decompose at temperatures as high as 485–545 °C. At a constant current density of 25 mA cm^?2, an ITO/BN₃/Al single‐layer device has a much‐longer lifetime (>80 h) than that of an ITO/NPB/Al single‐layer device (8 h). Also, the lifetime of a multilayer device based on BN₁ is longer than a similar device based on NPB. BNs are efficient and versatile OLED materials: they can be used as a hole‐transport layer (HTL), a host, and a deep‐blue‐light‐emitting material. This versatility may cut the cost of large‐scale material manufacture. More importantly, the deep‐blue electroluminescence (emission peak at 444 nm with CIE coordinates (0.16, 0.11), 3.23 cd A^?1 at 0.21 mA cm^?2, and 25200 cd m^?2 at 9 V) remains very stable at very high current densities up to 1000 mA cm^?2.     

Highly efficient single-layer organic light-emitting devices using cationic iridium complex as host

Highly efficient single-layer organic light-emitting devices (OLEDs) based on blended cationic Ir complexes as emitting layer have been demonstrated using narrow band gap cationic Ir complex [Ir(Meppy)₂(pybm)](PF₆) (C1) as guest and wide band gap cationic Ir complex [Ir(dfppy)₂(tzpy-cn)](PF₆) (C2) as host. As compared with single cationic Ir complex emitting layer, these host–guest systems exhibit highly enhanced efficiencies, with maximum luminous efficiency of 25.7 cd/A, external quantum efficiency of 8.6%, which are nearly 3-folds of those of pure C1-based device. Compared with a multilayer host-free device containing C1 as emitting layer and TPBI as electron-transporting and hole-blocking layer, the above single-layer devices also show 2-folds enhancement efficiencies. The high efficiencies achieved in these host–guest systems are among the highest values reported for ionic Ir complexes-based solid-state light-emitting devices. In addition, a white-similar emission with CIE of (0.36, 0.47) has also been achieved with luminous efficiency of 4.2 cd/A as the C1 concentration is 0.1 wt.%. The results demonstrate that the ionic Ir complexes-based host–guest system provides a new approach to achieve highly efficient OLEDs upon single-layer device structure and solution-processing technique.     

An efficient bis(2-phenylquinoline) (acetylacetonate) iridium(III)-based red organic light-emitting diode with alternating guest:host emitting layers

We report a highly efficient electrophosphorescent bis(2-phenylquinoline) (acetylacetonate) iridium(III) [Ir(2-phq)₂(acac)]-based red organic light-emitting diode. The emission layer consists of a periodic thin layer of guest material of Ir(2-phq)₂(acac) separated by host material of 4,4′-Bis(carbazol-9-yl)biphenyl. The guest and host thicknesses were optimized independently to obtain the best performance. The current efficiency reaches to a maximum of 16.2 cd/A then drops to 15 and 11 cd/A at brightness of 10 and 100 cd/m², respectively. By reducing the thickness of the host layer, the power efficiency was further improved. Device with a maximum power efficiency of 8.3 lm/W was obtained. We also found that the concentration quenching in Ir(2-phq)₂(acac) is dominated by molecular aggregation. Excitonic quenching by radiationless Förster process is miniscule.     

基于液晶衬垫的OLED光萃取

采用旋涂的方法制备了(3,4-亚乙二氧基噻吩) :聚(苯乙烯磺酸)(PEDOT:PSS)薄膜,结合液 晶衬垫(LCS,liquid crystal spacer)对OLED进行光萃取,制备了结构为Glass/ITO/PEDOT:P SS/LCS/NPB(40nm)/Alq₃(40nm)/LiF(1nm )/Al(100nm)的OLED以及其相应的对比 器件。通过测量其电压、 电流、亮度、色坐标和电致发光(EL)光谱等参数,研究了LCS对OLED发光性能 的影响。结果表明, 当引入LCS后,OLED在电压为11V时,最大电流效率达6.15cd/A,比不加 LCS的器件提高了40%;且在电压从7V上升到12V的过程中,器件的色坐标仅从(0.31,0.57) 变化到(0.31,0.56)。究其原因,LCS的引入可以提高透过率,破坏器 件内部光的折射以及全反射条件,并使功能层形成褶皱结构,使更多的光子能够从器件内发 射,也增大了电极的表面积,使电流密度增加,注入的能量提高。     

MoO3 as a cathode buffer layer for enhancing the efficiency in white organic light-emitting diodes

Molybdenum trioxide(MoO 3)as a cathode buffer layer is inserted between LiF and Al to improve the efficiency of white organic light-emitting diodes(OLEDs)in this paper.By changing the MoO 3 thickness,a higher current efficiency of 5.79 cd/A is obtained at a current density of 160 mA/cm2 for the device with a 0.8 nm-thick MoO 3 layer as the cathode buffer layer,which is approximately two times greater than that of the device without MoO 3.The mechanism for improving the device efficiency is discussed.Moreover,at a voltage of 13 V,the device with a 0.8 nm-thick MoO 3 layer achieves a higher luminance of 22370 cd/m2,and the Commission Internationale de I,Eclairage(CIE)color coordinate of the device with 1 nm-thick MoO 3 layer is(0.33,0.34),which shows the best color purity.Simple electron-only devices are tested to confirm the impact of the MoO 3 layer on the carrier injection.     

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。     

CdS薄层对有机电致发光器件性能的影响

将光电材料硫化镉(CdS)薄层插入到结构为ITO/NPB/Rubrene/NPB/DPVBi/Alq3/LiF/Al的白光有机发光器件(OLED)的Alq3和LiF之间,研究了CdS对OLED性能的影响。结果表明,0.1nm厚的CdS插入Alq3和LiF之间的器件性能最好。器件电压从7 V变化到14 V时,色度均在白光的中心区域;当电压为7V时,器件的最大电流效率为9.09cd/A;当电压为14V时,器件的最大亮度为16 370cd/m2。不加CdS时,当电压为8V时,器件的最大效率为5.16cd/A;当电压为14V时,最大亮度为6 669cd/m2。加CdS的器件比不加CdS的器件最大效率提高了1.76倍,最大亮度提高了2.42倍。     

加入激子阻挡层增强白色有机发光器件效率

通过在发光层（EBL）与电子注入层之间增加激子阻挡层（EBL）制备了新型白色有机发光器件（WOLED）。有EBL的新型器件效率和亮度均比传统结构器件高50％,在电流密度为4mA／cm^2时效率达到3．42cd／A,最大亮度为11000cd／m^2（16V）,色坐标为x=0．34、y=0．36;而具有相同EBL厚度的传统结构器件,在电流密度为4mA／cm^2时效率为2．15cd／A,最大亮度为6259cd／m^2（16V）。效率的提高是由于EBL的限制作用而提高了激子浓度。测量了器件的效率与电流密度关系,随电流密度增加电流效率的衰减缓慢,说明短寿命红色搀杂剂的激子-激子湮灭很弱。     

高效率磷光与荧光相结合的白色有机发光器件

制作了一种白色有机电致发光器件(WOLED)。将红光[Ir(piq)2(acac)]及绿光[Ir(ppy)3]磷光掺杂染料分别掺入到母体CBP中,在2种磷光发光层间插入蓝光材料DPVBi,引入电子传输能力强的BPhen作为电子注入层和空穴阻挡层,通过改变蓝光发光层的厚度,得到了高效率的WOLED,最大电流效率可达17.6cd/A,最大功率效率达13.7lm/W,最大亮度达27525cd/m2,当电压从4V变化到12V时,色坐标从(0.54,0.35)变化到(0.30,0.31),基本处于白光区。器件的特点在于DPVBi的存在阻挡了2种磷光材料间的能量转移,色度可以通过简单地调整DPVBi的厚度,避免使用稀有的蓝光磷光材料和与其相匹配的母体材料,同时又可以保持较高的发光效率。