Sr3(BN2)2荧光粉的合成与发光性能

采用高温固相一步法合成了新型荧光粉Sr_3(BN_2)_2(以下简写为SBN)。采用X射线衍射、扫描电子显微镜、荧光分光光度计对荧光粉的相组成、形貌和发光性能进行表征。讨论了SBN荧光粉的缺陷发光机理和长余辉特性。结果表明,所制备的样品SBN晶体为立方晶系Im-3m。在紫外区域有较宽的激发带,发射光谱峰值位于525 nm,半峰宽为3 334 cm~(-1)。SBN荧光粉材料存在本征缺陷,在基质中形成了Sr的空位,在光激励下形成发光中心。进一步的余辉衰减曲线与热释光曲线也证实,该材料存在固有缺陷,其余辉时间约10 s。变温光谱显示,当温度达到150℃时,荧光强度是室温初始强度的43%,优于稀土掺杂硼氮化物衰减到10%的结果。SBN荧光粉具有合成工艺简单、结构稳定、紫外波段激发获得长余辉绿光发射等优异性能,在LED发光器和指示方面具有潜在的应用前景。     

BaGa2Si2O8∶Eu^2+,Eu^3+,Pr^3+的发光性质及其防伪加密应用

采用高温固相法在单一基质中制备了具有多模态发光特性的系列荧光粉BaGa2Si2O8∶Eu2+,Eu3+,Pr3+,掺入适量的Pr3+可显著改善荧光粉的余辉发光性能。结果表明,该系列荧光粉在254 nm或365 nm的光激发下,具有不同颜色的光致发光和余辉发光,体现出多模发光特征;同时该系列荧光粉的余辉发光还具有不同的衰减时间。根据这些发光特性,选用合适的荧光粉制作了系列发光图案。相关典型应用示例表明,该发光图案的多模发光特征可应用于发光防伪应用,而基于其差异化的余辉衰减特性,还可以设计出可动态变化的余辉发光图案,从而增加发光防伪和加密的安全层级。     

CaS:Eu,Sm荧光粉表面二氧化硅包覆对其光激励发光特性的影响(英文)

改进了CaS∶Eu,Sm荧光粉在实时剂量计系统中的稳定性和实用性。以不同体积的正硅酸乙酯作为前驱体,采用溶胶凝胶法对CaS∶Eu,Sm荧光粉进行表面包覆。分别使用荧光分光光度计和酸度计对荧光粉的发光特性和防水特性进行表征。实验结果显示当质量分数为5%时,包覆层能明显提高荧光粉的稳定性且不影响荧光粉的发光强度。从材料的光激励发光和剂量响应测试实验中可以得出材料的退火特性以及相应的辐射剂量值。以CaS∶Eu,Sm荧光粉为基础的辐射剂量测试系统显示在0.1～300 Gy范围内具有良好的线性关系。结果显示表面包覆层明显抑制光激励发光特性,而且随着辐射剂量的增加,这种影响愈来愈显著。最后,我们提出了以光激励发光技术为基础的辐射剂量在线测试改进系统。     

长余辉发光材料的紫外-可见反射光谱测定

用“湿法”制备了长余辉发光材料,原料通过水溶液液相分子水平上的均匀混合,利用金属硝酸盐和有机还原剂在较低的温度下发生氧化还原燃烧反应,一步快速生成产品。加热起燃温度低至500℃,反应时间短,所制得的产品成份均匀,晶粒小,外观呈蓬松状态,易研磨粉碎,粉体表观密度小。以紫外－可见分光光度计测定分析了所制备样品在蓄光前后的反射光谱特征并作了探讨。结果表明,除表观密度外,“显法”与“干法”制备的长余辉发光材料的主要性质相同,紫外－可见反射光谱可以准确描述长余辉发光材料的紫外－可见光谱性能特征。     

长余辉荧光粉

据报导,日本千叶大学与齿科大学成功地合成了一种长余辉硅酸锌荧光粉,发光状态可持续30分钟左右。 硅酸锌,是一种具有代表性的荧光粉,常用在荧光灯和各种阴极射线管中,但是不具备这种长余辉特性。在硅酸锌中掺进微量的砷,可使之具有长余辉特性,这种荧光粉的合成容易,不受场合限制。而且通过原料成分的控制,可产生绿、黄、桃红三种颜色,稳定性好。目前实际使用的余辉性荧光基本属于硫化锌系,制备很困难。另外没有     

Sr3SiO5∶Eu^2＋和Sr3SiO5∶Eu^2＋,Dy^3＋荧光粉的黄色长余辉性质

用高温固相法制备了Sr3SiO5∶Eu2 和Sr3SiO5∶Eu2 ,Dy3 荧光粉。在紫外光辐照后,Sr3SiO5∶Eu2 和Sr3SiO5∶Eu2 ,Dy3 荧光粉具有明亮的黄色长余辉,源于Eu2 的4f65d-4f7的跃迁。紫外光激发停止后,Sr3SiO5∶Eu2 的余辉时间是4 h以上。余辉衰减曲线和热释光曲线说明了引入Dy3 离子可以产生大量的深陷阱和浅陷阱。产生的深陷阱使余辉时间延长到6 h以上。由热释发光曲线,根据热释光的通用级公式拟合了陷阱深度。Sr3SiO5∶Eu2 和Sr3SiO5∶Eu2 ,Dy3 荧光粉是有应用前景的黄色长余辉材料。     

纳米纤维状Sr3Al2O5Cl2∶Eu2+, Tm3+的白色长余辉性能

采用高温固相法在800 ℃下制备出系列白色长余辉荧光粉Sr3Al2O5Cl2∶Eu2+, Tm3+,并研究了它们的结构、形貌及发光性能.样品Sr2.91Al2O5Cl2∶0.04Eu2+, 0.05 Tm 3+具有单一晶相和纳米纤维结构.该样品在紫外光激发下表现出两个很强的宽带发射(分别位于~448 nm和~590 nm).它的余辉寿命大约是20 min.利用此种荧光粉所制作出的白光LED器件表现出很强的白光发射.     

彩色发光涂料的光学测量

彩色发光涂料是一种高光效、长余辉的光致发光材料。当对其进行光学测量时,为避免因激发光被探测器接收而对测量结果产生的影响,提出在实验中如何设定特殊的装置,从而保障对发光涂料的光学特性进行有效的测量。根据光度学理论中有关照度和发光亮度的关系,通过实验对三种不同的彩色发光涂料在同样光照条件下的亮度测量,同一种发光涂料在不同颜色光照下的发光亮度比较,以及在彩色发光涂料的亮度衰减情况给出了测量的结果。     

Sr3SiO5:Eu2+和Sr3SiO5:Eu2+, Dy3+荧光粉的黄色长余辉性质

用高温固相法制备了Sr3SiO5:Eu2 和Sr3SiO5:Eu2 , Dy3 荧光粉.在紫外光辐照后, Sr3SiO5:Eu2 和Sr3SiO5:Eu2 , Dy3 荧光粉具有明亮的黄色长余辉,源于Eu2 的4f65d - 4f7的跃迁.紫外光激发停止后,Sr3SiO5:Eu2 的余辉时间是4 h以上.余辉衰减曲线和热释光曲线说明了引入Dy3 离子可以产生大量的深陷阱和浅陷阱.产生的深陷阱使余辉时间延长到6 h以上.由热释发光曲线,根据热释光的通用级公式拟合了陷阱深度.Sr3SiO5:Eu2 和Sr3SiO5:Eu2 , Dy3 荧光粉是有应用前景的黄色长余辉材料.     

长余辉发光玻璃研究进展

介绍了长余辉发光玻璃的研究历程与进展，从长余辉发光玻璃的发展过程、发光机理、制备方法和发展现状等方面进行了分析，并对长余辉发光玻璃研究中存在的一些问题和发展方向提出了一些见解。     

基于紫外荧光技术的柴油机润滑油被燃油稀释的检测研究

针对柴油机润滑油被燃油稀释的状态监测的问题,研究了基于紫外荧光技术的柴油机润滑油被燃油稀释的检测方法,设计搭建了检测实验装置。利用峰值发射波长为365 nm的紫外LED作为发射光源,发射的紫外光通过400 nm低通滤光片过滤后进入石英比色皿中的油样,并激发油样产生荧光,产生的荧光通过400 nm高通滤光片过滤后,利用探测波长范围为400～800 nm的光电传感器采集油样的荧光信号,利用万用表读取油样的荧光强度。设计开发了信号的放大和测量系统。高、低通滤光片的组合使用,减少了紫外光源所发射的紫外光对油样的荧光强度测量的干扰。利用该实验装置,测量了润滑油中柴油含量分别为20.3 Wt.%,10.0 Wt.%,5.0 Wt.%,2.5 Wt.%,1.5 Wt.%和0.7 Wt.%以及不含柴油的空白油样的荧光强度,经拟合得到柴油含量与荧光强度的方程。最后,为了检验该方法测量润滑油中柴油含量的准确性,采用柴油含量为7.5 Wt.%油样进行验证,利用该实验装置,测量了验证油样的荧光强度,代入拟合方程,计算得到油样中的柴油含量,结果表明通过该方法测量的油样中柴油含量与油样的实际柴油含量的相对误差为0.5%,实现了实验室条件下润滑油被燃油稀释的精确测量。     

光导纤维反射光谱技术在彩绘文物颜料无损分析鉴定中的应用

文物颜料成分分析鉴定是文物材质分析和文物保护工作的重要内容。利用自行研制的光导纤维反射光谱仪对唐代彩绘陶器和壁画上的颜料成分进行了无损分析鉴定,通过比较彩绘文物颜料和标准颜料的反射光谱曲线的形状以及特征峰或一阶导数峰来完成颜料的鉴定工作。光导纤维反射光谱法鉴定出西安市唐代彩绘文物1#样品墓葬壁画上的深红色颜料是纯度较高的土红;2#样品陶器残片上的绿色颜料为石绿;3#样品陶缸残片上的橙红色和朱红色颜料分别是由大量铅丹和微量土红及大量朱砂和微量土红的混合物所组成。采用X射线荧光分析法进行验证,实验结果表明光导纤维反射光谱技术鉴定彩绘文物颜料成分的结果是准确、可靠的,提供了一种文物颜料无损分析的简捷方法。     

Analysis of Center Wavelength Shift of VCSEL Light in AWG for WDM PON Applications

Center wavelength shift of vertical cavity surface emitting laser light in arrayed waveguide gratings is verified with mathematical and experimental analysis.It is induced by the linearly increasing trend of optical power of vertical cavity surface emitting laser by bias current increase.It is retrieved effectively to the original center wavelength by simple correction method of compensation.This was done for application of vertical cavity surface emitting laser as a light source in optical line terminal of wavelength division multiplexing-passive optical network.     

基于双光导纤维延时法测量光速

介绍了利用光波在已知长度差的两段不同长度的光导纤维中传输时间延时差测量光速的基本原理。时钟方波信号通过LED调制电路转变为光信号在一段光导纤维中传输,后经SPD再生电路重新转变为方波再生信号,将原始方波信号与再生方波信号同时输入示波器中测量延时τ1,采用相同的方法测量另一端光导纤维传输延时τ2,通过已知的长度差和延时计算出光导纤维中的光速VZ,最终计算出光速c。     

用配光曲线作判据选择LED标准管

鉴于LED标准管具有量值传递方便进而统一量值的优点,指出作为标准管不仅要保证赋值的准确性和其量值保持长期稳定性,选择LED标准管要求其配光曲线要好,即接近朗伯发光体。介绍了配光曲线的概念及为得到配光曲线而使用的分布光度计;列举了可供选择的3种类型的电光源和选择LED标准管时接触到的10种典型配光曲线以及3种错误的配光曲线,在此基础上明确了选择LED发光质量好的白光管作为标准管的理由。     

Fabrication and comparison of thermochromic material-based fiber-optic sensors for monitoring the temperature of water

In this study, we explored the feasibility of developing two types of fiber-optic temperature sensors that can measure the temperature of water. One uses a thermochromic material such as Lophine, whose optical absorbance changes according to the thermal variation. The other uses a thermochromic pigment that gradually loses its own color through heat absorption. We measured the change in the intensity of the reflected light, which was due to the variation of the optical property of Lophine and pigments, with thermal variation. The relationship between the temperature of water and the output signal of the fiber-optic sensors was also determined. The fiber-optic temperature sensor using Lophine provided a relatively broad range of temperature measurement with low sensitivity, whereas the fiber-optic temperature sensor using a thermochromic pigment offered a high sensitivity in a narrow range of temperature measurement.     

Characterization of Particulate Mixtures by In-Line Measurments

The quality of particulate mixtures influences strongly the efficiency of downstream process steps. The design or optimization of mixing processes requires fast and accurate methods for determining mixture quality. This paper describes an optical method for the in-line concentration measurement of the key (tracer) component in particulate mixtures with fiber optical probes. Small fluctuations of tracer concentration equivalent to a low concentration variance represent a high degree of mixing. Monochromatic light penetrates via fiber optical probes into a powder sample. A photometer measures the intensity of the diffuse reflected light. If the tracer differs in colour from the other components of the mixture its concentration can be determined. Three types of fiber optical probes were tested. For calibration two series of mixed samples covering a broad concentration range were prepared, one consisting of white Al(OH)₃ and dark SiC and the other of Al(OH)₃ and a much finer green pigment. The calibration graphs are described by the Kubelka-Munk theory. The influence of changes in particle size on the signals is reduced by choosing a probe with an angled arrangement of the fibers. The sample mass of the probes is estimated to ca. 0.01 g, based on comparison with random mixtures at different tracer concentrations. In-line measurements provide extensive data sets which allow advanced statistical intepretations of mixing processes.     

高温物体比辐射率及温度测量系统

本文介绍了一种利用激光作为光源,利用遮蔽板作为标准噪声辐射源,并以８０３１ 单片机为核心实现测量静止及慢速运动的高温物体的比辐射率及温度系统。该系统主要由光学发射与接收系统、信号放大与处理系统及显示系统三部分组成。文中还详细介绍了该系统的工作原理与基本结构,讨论了其中的技术难点及其相应的解决方法,分析了各量的测量精度对比辐射率及温度测量精度的影响     

3.3-microm microcavity light emitter for gas detection

A room-temperature resonant-cavity light source emitting at 3.327 microm is presented. It combines a CdHgTe light-emitting layer, grown by molecular beam epitaxy, and two evaporated YF(3)-ZnS Bragg mirrors. The emitter is optically pumped by a commercial low-power GaAs laser diode. Compared with an unprocessed sample, this microcavity device shows a drastic (10-fold) linewidth reduction, a 3.3-fold intensity increase at 3.327 microm , and a 2.4-fold angular-spread decrease. The emitted optical power is 15 microW , and the device is used as a light source in a basic gas-detection setup. Measurements of a butane-propane mixture in the 1 to 5x 10(-3) bar range with a 5-cm-long single-path gas cell are demonstrated.     

Terahertz tomography using quantum-cascade lasers

The interfaces of a dielectric sample are resolved in reflection geometry using light from a frequency agile array of terahertz quantum-cascade lasers. The terahertz source is a 10-element linear array of third-order distributed-feedback QCLs emitting at discrete frequencies from 2.08 to 2.4 THz. Emission from the array is collimated and sent through a Michelson interferometer, with the sample placed in one of the arms. Interference signals collected at each frequency are used to reconstruct an interferogram and detect the interfaces in the sample. Because of the long coherence length of the source, the interferometer arms need not be adjusted to the zero-path delay. A depth resolution of 360 μm in the dielectric is achieved with further potential improvement through improved frequency coverage of the array. The entire experiment footprint is <1 m×1 m with the source operated in a compact, closed-cycle cryocooler.