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1.
红绿掺杂有机电致发光器件发光性能的研究   总被引:2,自引:2,他引:0  
制备了结构为ITO/MoO3(x nm)/NPB(40nm)/CBP:14%GIr1(12.5nm)/CBP:6%R-4b(5nm)/C BP:14% GIr1(12.5nm)/BCP(10nm)/Alq3( 40nm)/LiF(1nm)/Al(100nm)的红绿磷光器件,G Ir1和R-4B分别为新型绿色和 红色磷光染料,采用绿-红-绿掺杂顺序,结合BCP对空穴的有效限制作用,研究了不同MoO 3厚度器件的发光 机理。结果表明,在MoO3为40nm时,器件发光性能较好,在电压 为5V、亮度为100cd·m-2时,得到最大的 电流效率为16.91cd·A-1。为提高器件光效,增加TCTA电子 阻挡层,获得了最高电流效率20.01cd·A-1。原因主要是, TCTA的HOMO能级介于NPB和CBP之间,促进空穴注入;TCTA较高的三线态能量对发光层激子的 限制。  相似文献   

2.
间隔层提高有机电致发光器件的性能   总被引:3,自引:3,他引:0  
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。  相似文献   

3.
蓝绿色磷光OLED的制备及发光性能研究   总被引:4,自引:4,他引:0  
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。  相似文献   

4.
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。  相似文献   

5.
有机电致发光器件的发光颜色与色纯度在很大程度上受限于有机材料本身特性,而通过光学微腔效应可以从器件结构的改变来进行色纯度的调节。本文介绍了一种通过调节有机结构中空穴传输层和电子阻挡层厚度,从而改变器件微腔腔长,获得高纯度顶发射单色发光器件的方法。利用这种方法制作的有机顶发射绿色磷光器件结构为Si Substrate/Ag/ITO/ NPB: F16CuPc(10 nm, 3%)/NPB(x nm)/ TCTA(y nm)/ mCP: Ir(ppy)3(40 nm, 6%)/ Bphen: Liq(30 nm, 40%)/Mg: Ag(12 nm, 10%)/Alq3(35 nm),改变NPB和TCTA的厚度,获得了高色纯度发光器件,正向出射绿光的色坐标达到(0.2092,0.7167),接近标准绿光(0.21, 0.71)。  相似文献   

6.
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(y1nm)/ CBP:Ir(ppy)3(x%,y nm)/TPBi(y2nm)/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)。  相似文献   

7.
绿红双发光层有机电致磷光器件的载流子调控研究   总被引:4,自引:1,他引:3  
制备了结构为ITO/MoO3(40nm)/NPB(40nm)/TCTA(10nm)/CBP∶GIR1(14%)(x)/CBP∶R-4B(6%)(30-x)/BCP(10nm)/AlQ(40nm)/LiF(1nm)/AL(100nm)的绿红磷光器件。通过调节红绿发光层的相对厚度,对器件的发光性能进行了研究。结果表明:x为15nm,电压为6V,电流密度为255.6mA/cm2,得到最高电流效率为15.4cd/A,红色发光峰值强度相对较大,绿色峰值稍弱的电致发光光谱。分析原因可能是掺杂染料与临近层的能级匹配和浓度等会影响发光层载流子注入与传输;空穴及电子阻挡层对发光层内载流子和激子的有效限制作用会提高掺杂染料在发光层的复合几率;另外,CBP的空穴迁移率大于电子迁移率,发光的主要区域位于发光层与BCP界面,掺杂于该区域的R-4B具有较高的发光强度。  相似文献   

8.
张静  张方辉 《光电子.激光》2012,(11):2056-2060
使用绿色磷光材料GIr1作为掺杂剂,制备了基于CBP材料的一系列绿色有机电致发光器件(OLED)。其器件的结构为ITO/MoO3(50nm)/NPB(40nm)/TCTA(10nm)/CPB:GIr1(30nm,x%)/BCP(10nm)/Alq3(20nm)/LiF(1nm)/Al(100nm),其中x%为发光层客体掺杂质量分数。对7种不同的掺杂剂质量分数进行了比较,研究了它们的电致发光(EL)特性。结果显示,对发光面积为2.72cm2的器件,GIr1的最佳掺杂比为14%,器件的起亮电压为3.5V,器件的最大电流效率26.2cd/A,其相应的EL主峰位于524nm,色坐标为(0.34,0.61),得到了发光性能稳定的绿色OLED。  相似文献   

9.
杜帅  张方辉  程君  李怀坤 《光电子.激光》2015,26(10):1878-1884
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。  相似文献   

10.
磷光与荧光相结合的多层白色有机发光器件   总被引:2,自引:2,他引:0  
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。  相似文献   

11.
DUV lithography, using the 248 nm wavelength, is a viable manufacturing option for devices with features at 130 nm and less. Given the low kl value of the lithography, integrated process development is a necessary method for achieving acceptable process latitude. The application of assist features for rule based OPC requires the simultaneous optimization of the mask, illumination optics and the resist.Described in this paper are the details involved in optimizing each of these aspects for line and space imaging.A reference pitch is first chosen to determine how the optics will be set. The ideal sigma setting is determined by a simple geometrically derived expression. The inner and outer machine settings are determined, in turn,with the simulation of a figure of merit. The maximum value of the response surface of this FOM occurs at the optimal sigma settings. Experimental confirmation of this is shown in the paper.Assist features are used to modify the aerial image of the more isolated images on the mask. The effect that the diffraction of the scattering bars (SBs) has on the image intensity distribution is explained. Rules for determining the size and placement of SBs are also given.Resist is optimized for use with off-axis illumination and assist features. A general explanation of the material' s effect is discussed along with the affect on the through-pitch bias. The paper culminates with the showing of the lithographic results from the fully optimized system.  相似文献   

12.
From its emergence in the late 1980s as a lower cost alternative to early EEPROM technologies, flash memory has evolved to higher densities and speedsand rapidly growing acceptance in mobile applications.In the process, flash memory devices have placed increased test requirements on manufacturers. Today, as flash device test grows in importance in China, manufacturers face growing pressure for reduced cost-oftest, increased throughput and greater return on investment for test equipment. At the same time, the move to integrated flash packages for contactless smart card applications adds a significant further challenge to manufacturers seeking rapid, low-cost test.  相似文献   

13.
The relation between the power of the Brillouin signal and the strain is one of the bases of the distributed fiber sensors of temperature and strain. The coefficient of the Bfillouin gain can be changed by the temperature and the strain that will affect the power of the Brillouin scattering. The relation between the change of the Brillouin gain coefficient and the strain is thought to be linear by many researchers. However, it is not always linear based on the theoretical analysis and numerical simulation. Therefore, errors will be caused if the relation between the change of the Brillouin gain coefficient and the strain is regarded as to be linear approximately for measuring the temperature and the strain. For this reason, the influence of the parameters on the Brillouin gain coefficient is proposed through theoretical analysis and numerical simulation.  相似文献   

14.
The parallel thinning algorithm with two subiterations is improved in this paper. By analyzing the notions of connected components and passes, a conclusion is drawn that the number of passes and the number of eight-connected components are equal. Then the expression of the number of eight-connected components is obtained which replaces the old one in the algorithm. And a reserving condition is proposed by experiments, which alleviates the excess deletion where a diagonal line and a beeline intersect. The experimental results demonstrate that the thinned curve is almost located in the middle of the original curve connectivelv with single pixel width and the processing speed is high.  相似文献   

15.
Today, micro-system technology and the development of new MEMS (Micro-Electro-Mechanical Systems) are emerging rapidly. In order for this development to become a success in the long run, measurement systems have to ensure product quality. Most often, MEMS have to be tested by means of functionality or destructive tests. One reason for this is that there are no suitable systems or sensing probes available which can be used for the measurement of quasi inaccessible features like small holes or cavities. We present a measurement system that could be used for these kinds of measurements. The system combines a fiber optical, miniaturized sensing probe with low-coherence interferometry, so that absolute distance measurements with nanometer accuracy are possible.  相似文献   

16.
This paper presents a new method to increase the waveguide coupling efficiency in hybrid silicon lasers. We find that the propagation constant of the InGaAsP emitting layer can be equal to that of the Si resonant layer through improving the design size of the InP waveguide. The coupling power achieves 42% of the total power in the hybrid lasers when the thickness of the bonding layer is 100 nm. Our result is very close to 50% of the total power reported by Intel when the thickness of the thin bonding layer is less than 5 nm. Therefore, our invariable coupling power technique is simpler than Intel's.  相似文献   

17.
A new quantum protocol to teleport an arbitrary unknown N-qubit entangled state from a sender to a fixed receiver under M controllers(M < N) is proposed. The quantum resources required are M non-maximally entangled Greenberger-Home-Zeilinger (GHZ) state and N-M non-maximally entangled Einstein-Podolsky-Rosen (EPR) pairs. The sender performs N generalized Bell-state measurements on the 2N particles. Controllers take M single-particle measurement along x-axis, and the receiver needs to introduce one auxiliary two-level particle to extract quantum information probabilistically with the fidelity unit if controllers cooperate with it.  相似文献   

18.
A continuous-wave (CW) 457 nm blue laser operating at the power of 4.2 W is demonstrated by using a fiber coupled laser diode module pumped Nd: YVO4 and using LBO as the intra-cavity SHG crystal With the optimization of laser cavity and crystal parameters, the laser operates at a very high efficiency. When the pumping power is about 31 W, the output at 457nm reaches 4.2 W, and the optical to optical conversion efficiency is about 13.5% accordingly. The stability of the out putpower is better than 1.2% for 8 h continuously working.  相似文献   

19.
It is well known that adding more antennas at the transmitter or at the receiver may offer larger channel capacity in the multiple-input multiple-output(MIMO) communication systems. In this letter, a simple proof is presented for the fact that the channel capacity increases with an increase in the number of receiving antennas. The proof is based on the famous capacity formula of Foschini and Gans with matrix theory.  相似文献   

20.
Call for Papers     
正Wireless Body-area Networks The last decade has witnessed the convergence of three giant worlds:electronics,computer science and telecommunications.The next decade should follow this convergence in most of our activities with the generalization of sensor networks.In particular with the progress in medicine,people live longer and the aging of population will push the development of wireless personal networks  相似文献   

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