彩色PDP中荧光粉发光色坐标的测量方法研究

等离子体显示器已成为平板显示领域主要发展方向之一。在等离子体显示器上测得的色坐标包含了两部分：一部分是荧光粉在PDP器件中发光色的色坐标，一部分是PDP工作时气体放电的色坐标。在PDP屏的制作过程中，荧光粉经历了浆料制备、干燥、烧结以及老炼等工艺过程。因此，荧光粉在PDP屏上表现出的色坐标比起荧光粉体来说会产生一些变化。本文以测量PDP中荧光粉发光色坐标为目的，提出了一种用单色PDP屏色坐标、亮度和同结构下气体放电色坐标、亮度来获得荧光粉在PDP屏中色坐标和亮度的方法，设计制作了测试PDP屏三基色荧光粉发光色坐标所用的单色试验屏。用CRT ColorAnalyzer（CA－100）时PDP屏和PDP屏上气体放电产生的亮度和色坐标都进行了测量，根据合成颜色的在刺激值与二种已知颜色的在刺激值具有线性叠加关系，计算出了荧光粉在PDP器件中的色坐标和亮度。同时，用WGD－3型组合式多功能光栅光谱仪对PDP屏和气体放电的发光光谱进行了测量，用计算机将测得的发光光谱在同波长下相减，从而获得了荧光粉在PDP中的发光光谱。结果表明绿粉和蓝粉的色坐标变化较大，而红粉变化较小，使得PDP白场色温向较低的方向变化。绿粉和蓝粉的发光谱线的半峰宽与原粉比较都有减小，峰值发光强度也减小了，绿粉的峰值发光波长从526nm变至523．4nm。     

(Zn,Cd)S∶Cu,Cl发光材料的热释发光

在ZnS中分别掺杂质量分数为5%、7%、10%、15%、20%的CdS,得到一系列(Zn,Cd)S∶Cu,Cl粉末电致发光材料样品。测量样品材料的热释发光曲线,发现五个样品在温度-180～-20℃范围内均有两个明显的热释发光峰。CdS含量的变化对材料中陷阱的种类和陷阱深度没有明显的影响,两个峰值温度在-150℃和-50℃附近。Cd离子的掺入改变了材料较深陷阱中载流子的浓度,随着CdS量的增加,使得在-50℃的热释发光峰的相对强度增大。通过测量样品的发光光谱和发光亮度,发现随着CdS含量的增加,样品材料的发射光谱向长波方向移动,发光亮度呈下降的趋势。     

(Zn,Cd)S：Cu,Cl发光材料的热释发光

在ZnS中分别掺杂质量分数为5%、7%、10%、15%、20%的CdS,得到一系列(Zn,Cd)S:Cu,Cl粉末电致发光材料样品。测量样品材料的热释发光曲线,发现五个样品在温度-180～-20℃范围内均有两个明显的热释发光峰。CdS含量的变化对材料中陷阱的种类和陷阱深度没有明显的影响,两个峰值温度在-150℃和-50℃附近。Cd离子的掺入改变了材料较深陷阱中载流子的浓度,随着CdS量的增加,使得在-50℃的热释发光峰的相对强度增大。通过测量样品的发光光谱和发光亮度,发现随着CdS含量的增加,样品材料的发射光谱向长波方向移动,发光亮度呈下降的趋势。     

以蓝色发光材料DPVBi为基质的白色发光器件

白色有机发光器件是实现彩色平板显示的重要方案之一。利用蓝色发光材料DPVBi[4，4′—(2，2—苯乙烯基)—1，1′—联苯]掺杂红光染料DCJTB[4—氰甲烯基—2—叔丁基—6—(1，1，7，7—四甲基久洛尼定基—9—烯炔基—4H—吡喃)]作发光层制备了白色发光器件。研究了DPVBi掺杂不同浓度IDCJTB薄膜的光致发光性质，根据光致发光结果，制备了以DPVBi掺杂不同浓度DCJTB作发光层的电致发光器件，其结构为ITO／GuPc／NPB／DPVBi：DCJTB／Alq3／LiF／Al。当DCJTB质量分数为0．0008时，器件实现了白色发光(色度x=0．25，y=0．32)，电致发光和光致发光的掺杂比例基本相符，表明器件的白色发光主要是由基质DPVBi向掺杂剂DCJTB的能量传递产生的。研究还发现：白色器件随电压升高，光谱中蓝色成分相对于红色成分的比例略有增加，文章对此现象进行了分析。该白光器件在14V时达到最高亮度7822cd／cm^2，在20mA／cm^2电流密度下的亮度为-489cd／cm^2，最大流明效率为1．75lm／W。     

白光光学信息处理及其彩色摄影术

本文阐述了白光光学信息处理的物理基础,给出了近十年来应用所研制的仪器和设备在实际应用中取得的结果。提出了一种新型数码相机的方案和彩色档案存储的新技术并为大学高等物理提供了一个现代光学和数字图像的实验素材。     

掺杂Gd^3＋对Y2O2S：Eu^3＋发光特性的影响

在红色荧光粉Ｙ２Ｏ２Ｓ：Ｅｕ＾３＋的制备过程中掺入了不同浓度的Ｇａ２Ｏ３;发现在掺入适当浓度的Ｇａ２Ｏ３的情况下,可以增强发射强度并改善其电压特性,即在保证所要求的发光颜色、粒径和其它物理及化学特性的条件下,可改善发射强度与激发电压间的关系,讨论和分析了强度被增强的起因。Ｇａ＾３＋对Ｙ＾３＋的置换,减少了因Ｅｕ＾３＋对Ｙ＾３＋转换所引起的晶格的畸变,从而减弱了无辐射过程及因晶格畸变所造成的能量损失     

基于LabVIEW的发光微生物测量实验

论述了发光微生物的发光机理及基于LabVIEW的发光微生物测量原理,并在此基础之上,探讨了如何利用LabVIEW开发平台开发出发光微生物传感器虚拟仪器实验系统. 同时对LabVIEW软件以及信号采集卡进行必要的介绍.     

流场刺激下海洋生物发光的光学特性及数理模型

生物受激发光探测是一种感知水中目标的新技术、新手段。选取多边膝沟藻、夜光虫和月芽形梨甲藻3种典型海洋受激发光生物体为对象,采用光谱仪、光子计数器、库埃特流场旋转圆筒等装置搭建了生物受激发光实验平台,研究了不同刺激下生物体受激发光的光学特性,并在此基础上结合概率论和数理统计理论,建立了流场刺激下的生物发光的数理模型。结果表明:发光藻的发光具有较好的单色谱特性,峰值波长集中在472 nm左右,谱线的半波宽度为30～40 nm。发光藻的发光随着机体的疲劳而变弱,但发光能力随着机体的休息会慢慢恢复。同种刺激条件下,3种藻发光强度的强弱依次为月芽形梨甲藻、夜光虫、多边膝沟藻。     

Metal nanoparticle-doped coloured films on glass and polycarbonate substrates

In a program on the development of metal (e.g. Au, Ag, Cu and their alloy) nanoparticles in sol-gel derived films, attempts were made to synthesize different coloured coatings on glasses and plastics. The absorption position of surface plasmon resonance (SPR) band arising from the embedded metal nanoparticles was tailored by controlling the refractive index of the matrix for the development of different colours. Thus different coloured (pink to blue) coatings on ordinary sheet glasses were prepared by generating Au nanoparticles in mixed SiO₂-TiO₂ matrices having refractive index values ranging from about 1.41 to 1.93. In another development,in situ generation of Ag nanoparticles in the inorganic-organic hybrid host leads to the formation of different abrasion resistant coloured coatings (yellow to pink) on polycarbonate substrates after curing. As expected, the SPR peak of Ag or Au is gradually red-shifted due to the increase of refractive index of the coating matrices causing a systematic change of colour     

车用回复反射器光度性能测试方法研究

介绍了一种检测汽车回复反射器光度性能的测试系统的结构和原理。该测试系统采用激光束准直定位技术来确定回复反射器的位置 ,通过类似车灯灯光的集束光投射到回复反射器 ,利用高灵敏度的光度探测器检测反射器反射到各方向上的反射光强度。光度计测试范围为 10 - 6～ 1.999lx,激光束光斑口径为 5～ 9mm。整个系统由计算机控制 ,可以按国家标准自动完成测试。     

Stochastic resonance driven by time-modulated correlated coloured noise sources in a single-mode laser

This paper investigates the phenomenon of stochastic resonance in a single-mode laser driven by time-modulated correlated coloured noise sources. The power spectrum and signal-to-noise ratio R of the laser intensity are calculated by the linear approximation. The effects caused by noise self-correlation time τ₁, τ₂ and cross-correlated time τ₃ for stochastic resonance are analysed in two ways: τ₁, τ₂ and τ₃ are taken to be the independent variables and the parameters respectively. The effects of the gain coefficient Γ and loss coefficient K on the stochastic resonance are also discussed. It is found that besides the presence of the standard form and the broad sense of stochastic resonance, the number of extrema in the curve of R versus K is reduced with the increase of the gain coefficient Γ.     

Output power spectrum of a single-mode laser driven by coloured pump and quantum noises with coloured correlation

By using the linear approximation method, the output power spectrum is calculated for a single-mode laser driven by coloured pump and quantum noises with coloured correlation. We have observed that the configuration of the output power spectrum is complicated: that is, it can be of single peak, two peaks or three peaks. The configurations of the power spectrum can be transformed from one into another by changing the cross-correlation time, the cross-correlation coefficient between the two noises, and pump noise intensity.     

Statistical properties of a single-mode laser driven by additive and multiplicative coloured noises with a coloured cross-correlation for different correlation times

We study a system for a single-mode laser driven by additive and multiplicative coloured noises with a coloured cross-correlation. The analytical expression of the stationary intensity distribution (SID) for the laser is derived in the case of three different correlation times. The influences of each stochastic parameter on the SID are discussed, the effects of the noise "colour" and the cross-correlation of noises on the mean intensity , the variance, λ_2(0), and the skewness,λ_3(0) of the single-mode laser are investigated. We find that there are colourful phase transitions for the SID above a threshold, and re-entrant transitions induced by the "colour" of the additive noises. Further research of the curves of -τ_i, λ_2(0)-τ_i, and λ_3(0)-τ_i (i=1,2,3) (where τ_i is the correlation time) shows that the output intensity not only increases with the additive noise correlation time τ_2 and the cross-correlation time τ_3, but also the quality of the output of laser beams is optimized.     

Effects of signal modulation and coloured cross-correlation of coloured noises on the diffusion of a harmonic oscillator

The diffusion in a harmonic oscillator driven by coloured noises $\xi(t)$ and $\eta(t)$ with coloured cross-correlation in which one of the noises is modulated by a biased periodic signal is investigated. The exact expression of diffusion coefficient d as a function of noise parameter, signal parameter, and oscillator frequency is derived. The findings in this paper are as follows. 1) The curves of d versus noise intensity D and d versus noises cross-correlation time $\tau_3$ exist as two different phases. The transition between the two phases arises from the change of the cross-correlation coefficient $\lambda$ of the two Ornstein--Uhlenbeck (O-U) noises. 2) Changing the value of $\tau_3$, the curves of d versus Q, the intensity of colored noise that is modulated by the signal, can transform from a phase having a minimum to a monotonic phase. 3) Changing the value of signal amplitude A, d versus Q curves can transform from a phase having a minimum to a monotonic phase. The above-mentioned results demonstrate that a like noise-induced transition appears in the model.     

Formation and instability of spiral wave induced by Gaussian coloured noise

In this paper, we studied the effect of Gaussian coloured noise on the formation and instability of spiral waves described by one class of modified FitzHugh--Nagumo equation. It was found that Gaussian coloured noise plays a constructive role in the formation, transition and instability of spiral wave. Too weak or too strong noise may act against the formation of spiral waves. At a certain noise level, spiral wave is maintained in a medium, in which spiral wave cannot be observed in the absence of the noise. It is difficult to make a stable spiral wave into unstable state by Gaussian coloured noise, unless the noise level is very high. The parameter regions of Gaussian coloured noise for spiral forming and spiral instability were given and discussed with numerical simulations.     

Stochastic resonance in an asymmetric bistable system driven by coloured noises

The phenomenon of stochastic resonance is investigated in an asymmetric bistable system with coloured noises.The approximate Fokker-Planck equation is derived based on the Novikov theorem and the Fox approach.By applying the two-state theory,the expression of the signal-to-noise ratio is obtained in the adiabatic limit.The effects of the noise parameters on signal-to-ratio are discussed.It is found that the stochastic resonance phenomena appear in most cases and disappear in some special cases.     

Transitions in a genotype selection model driven by coloured noises

This paper investigates a genotype selection model subjected to both a multiplicative coloured noise and an additive coloured noise with different correlation time τ1 and τ2 by means of the numerical technique. By directly simulating the Langevin Equation, the following results are obtained. （1） The multiplicative coloured noise dominates, however, the effect of the additive coloured noise is not neglected in the practical gene selection process. The selection rate μ decides that the selection is propitious to gene A haploid or gene B haploid. （2） The additive coloured noise intensity and the correlation time τ2 play opposite roles. It is noted that α and τ2 can not separate the single peak, while can make the peak disappear and ~-2 can make the peak be sharp. （3） The multiplicative coloured noise intensity D and the correlation time τ1 can induce phase transition, at the same time they play opposite roles and the reentrance phenomenon appears. In this case, it is easy to select one type haploid from the group with increasing D and decreasing τ1.