荧光粉比例对白光LED特性的影响

用黄色和橙色硅酸盐荧光粉制备了白光LED,调整黄粉和橙粉的比例得到不同的色温.对样品进行光学测试,发现黄粉与橙粉的比例小于7时,黄光部分的峰值约590 nm,比例大于7时,黄光部分的峰值约570 nm;显色指数和流明效率都是随色温的增大先上升后下降,5521 K时达到最优值,这是由于低色温时,荧光粉的浓度大导致不能有效...     

Mössbauer effect study of γ-FeMn alloys

The disordered antiferromagnetic γ-FeMn alloys in the range of Mn concentration from 0 up to 50 at.% Mn were investigated by means of X-ray diffraction analysis (XRD), differential scanning calorimeter (DSC) and Mössbauer spectroscopy (ME) at room temperature and at 80 K. The lattice parameter is constant for Mn contents below 27 at.% and increases linearly for higher Mn concentration. The RT Mössbauer spectra for the alloys with less than 20 at.% Mn were fitted with quadrupole splitting (QS) distribution, and above 20 at.% Mn they were fitted with magnetic hyperfine field (HF) distribution. The averageQS decreases, while the HF maintain a constant value by increasing the Mn concentration. At 80 K, the HF increases linearly up to 30 at.% Mn and then maintains a constant value at about 38 kOe. The peak of the specific heat (c _p) at the Néel temperature changes from broad to sharp as the Mn content increases. The Néel temperature increases with Mn concentration.     

掺铬钛酸锶晶体的氧化还原诱导吸收及发光的退火效应和浓度效应

制备了纯的、掺0.005、0.01、0.2和0.5wt%Cr2O3的钛酸锶单晶.测量了不同退火条件下的室温透射光谱及6.5K以上的荧光光谱.对晶体的氧化和还原热处理诱导吸收及退火和掺杂浓度对晶体发光的影响进行了较为详细的研究.     

退火处理对YMnO3薄膜的结构和荧光性能的影响

室温下,采用脉冲激光沉积方法在Si(100)衬底上制备了YMnO3薄膜,并对其进行了不同温度的退火处理。采用X射线衍射和荧光光谱分析方法对薄膜的结构和荧光特性进行了研究。结果表明:通过退火处理,可以得到正交相和六方相共存的多晶态YMnO3薄膜,并且随着退火温度的升高,两相的比例发生变化,由正交相为主转变为六方相为主。YMnO3薄膜样品的荧光发射峰集中在波长430～620nm范围内,可能是由Mn3 离子从5T2到5E之间的能级跃迁所引起的。其荧光强度随着退火温度的升高逐渐增强,但峰位基本保持不变,说明薄膜结构的改变对Mn3 离子的能级跃迁几率有明显的影响,对能级位置的影响不大;而且荧光光谱还显示在同一薄膜中各个荧光峰的相对强度随着退火温度的变化不大。     

Thermo-stimulated luminescence of x-ray- and alpha-irradiated yttria-stabilized zirconia

Yttria-stabilized zirconia (ZrO2 : Y3+) single crystals (with 9.5 mol% Y2O3) were irradiated with x-rays and α particles. Thermally stimulated luminescence (TSL) data show a main broad peak centred at ～500-550 K in the glow curves of all irradiated samples. The TSL peak maximum temperature is consistent with the characteristic recovery temperature (～450 K) of colour centres (T centres) deduced from isochronal annealing curves measured by electron paramagnetic resonance (EPR) spectroscopy. However, the trap-depth energies (ranging between 0.8 and 1.2 eV) deduced from the initial rise of partially cleaned TSL peaks (and from a rough approximation using Urbach's formula) are much larger than the activation energies for defect recovery of 0.3 eV deduced from the EPR data. A second TSL peak centred at ～350-450 K found in freshly irradiated samples is seen to decay substantially in aged samples. The processes involved in TSL are discussed in relation to the defect annealing processes, and available defect-level energy and TSL data.     

Room-temperature fluorescence of a charge-transfer complex of reserpine in aqueous and aqueous–ethanol media

The room-temperature fluorescence of a charge-transfer (CT) complex different from those of the component donor/acceptor in polar organic solvent is not very common. The phenomenon is even rarer in aqueous medium. The present work demonstrates that a CT complex formed between reserpine (Res) and 2,3-dichloro-5,6-dicyano-1,4-benzoquinone (DDQ) in aqueous and aqueous–ethanol media exhibits fluorescence at room temperature that is entirely different from those of the components, Res and DDQ. With decreasing polarity of the medium on the addition of ethanol, the fluorescence intensity and also the fluorimetrically determined formation constant of the complex increase, but the fluorescence emission wavelength does not change significantly. The quantum yield of fluorescence of the CT complex systematically decreases with increasing ethanol content of the medium. That the observed fluorescence is due to the CT complex is established by the constancy of the assumed proportionality constant (β) between the fluorescence intensity and the complex concentration measured using different equilibrium concentrations of the complex and also by demonstrating the mirror image relationship between its excitation and emission spectra in aqueous medium. To our knowledge, this is the first report on the room-temperature fluorescence of a CT complex in aqueous solution.     

高压条件下酪氨酸在线荧光光谱研究

在Cu2+与酪氨酸摩尔浓度比为0至40范围内,考察了压力对酪氨酸荧光光谱的影响,结果表明:在无Cu2+情况下,压力对酪氨酸荧光强度具有增敏作用,压力越高,增敏效果越显著,当压力为60 MPa时,荧光强度增加了约9%.Cu2+对酪氨酸荧光有猝灭作用,Cu2+浓度越高,猝灭越强;在Cu2+存在的情况下,压力对酪氨酸荧光的影...     

Cd3Al2Ge3O12:Mn2+锗酸盐石榴石光谱性质

本文报道室温下Cd₃Al₂Ge₃O₁₂:Mn²⁺(简称CAGG:Mn²⁺)锗酸盐石榴石的漫反射光谱、激发和发射光谱.在UV光激发下,在CAGG中Mn²⁺离子发射强黄光,这是基质到Mn²⁺离子无辐射能量传递的结果.Mn²⁺的黄发射带是由一个弱的红带和一个强的绿带所组成.讨论了这两个Mn²⁺发射带的起因.     

The optical properties and energy transition process in nanocomposite of polyvinyl-pyrrolidone polymer and Mn-doped ZnS

This study has been carried out on the optical properties of polyvinyl-pyrrolidone (PVP), the energy transition process in nanocomposite of PVP capped ZnS:Mn nanocrystalline and the influence of the PVP concentration on the optical properties of the PVP capped ZnS:Mn nanocrystalline thin films synthesized by the wet chemical method. The microstructures of the samples were investigated by X-ray diffraction, the atomic absorption spectroscopy, and transmission electron microscopy. The results showed that the prepared samples belonged to the sphalerite structure with the average particle size of about 2–3 nm. The optical properties of samples are studied by measuring absorption, photoluminescence (PL) spectra and time-resolved PL spectra in the wavelength range from 200 to 700 nm at 300 K. From data of the absorption spectra, the absorption edge of PVP polymer was found about of 230 nm. The absorption edge of PVP capped ZnS:Mn nanoparticles shifted from 322 to 305 nm when the PVP concentration increases. The luminescence spectra of PVP showed a blue emission with peak maximum at 394 nm. The luminescence spectra of ZnS:Mn–PVP exhibits a blue emission with peak maximum at 437 nm and an orange–yellow emission of ion Mn²⁺ with peak maximum at 600 nm. While the PVP coating did not affect the microstructure of ZnS:Mn nanomaterial, the PL spectra of the PVP capped ZnS:Mn samples were found to be affected strongly by the PVP concentration.     

卤磷酸钙荧光粉中CaSb2O6:Mn的光谱研究

CaSb2O6:Mn是卤磷酸钙荧光粉(以下简称卤粉)中的杂质相,它对卤粉的发光性能和老化性能都有不良影响,这方面的研究已有较多论述。有关CaSb2O6:Mn的光谱研究尚不多。1951年曾发现在卤粉中增加Sb量时出现绿色发光。1955年R.Bernara曾描述了在520nm具有辐射的CaSb2O6:Mn的发光性质。     

Temperature and concentration effects in electron-stimulated desorption of sodium atoms from sodium layers adsorbed on tungsten coated with a gold film

The yield and energy distributions of sodium atoms upon electron-stimulated desorption from sodium layers adsorbed on tungsten coated with a gold film are investigated for the first time as functions of the thickness of the gold film, the concentration of deposited sodium, and the surface temperature. It is found that the energy distributions exhibit two peaks, namely, a narrow peak with a maximum at about 0.15 eV, whose intensity continuously increases with increasing temperature, and a broad peak with a maximum at about 0.35 eV, whose intensity either decreases or remains constant with increasing temperature. It is shown that both peaks arise as a result of the same excitation, which gives rise to different channels of electron-stimulated desorption of sodium atoms. Possible mechanisms of electron-stimulated desorption and the kinetics of destruction of the surface coating are discussed.     

TiO2微粒对远程荧光粉膜及白光发光二极管器件光色性能的影响

利用热压法将TiO₂微粒掺入至YAG:Ce荧光粉和硅树脂中制备出远程荧光粉膜并封装成白光发光二极管(LED)器件, 通过荧光粉相对亮度仪、双积分球测试系统和可见光光谱分析系统对样品的光色性能及机理进行了研究. 结果表明: TiO₂的散射效应能够显著提高蓝光的利用率和黄光的透射强度, 白光LED器件的光通量在TiO₂浓度为0.966 g/cm³ 时达到最高值415.28 lm(@300 mA, 9.3 V), 提高了8.15%, 相关色温从冷白6900 K逐渐变化至暖白3832 K. TiO₂的掺入不仅提高了远程荧光粉膜的发射强度和白光LED器件的光通量, 同时能调控其相关色温.     

Dy~(3+)掺杂硼酸盐玻璃的制备、表征及发光特性

采用高温熔融-冷却法制备了一系列Dy~(3+)掺杂的B_2O_3-ZnO-Na_2O-Al_2O_3发光玻璃,通过红外光谱、紫外-可见-近红外光谱和荧光光谱等研究了其结构及发光特性。分析表明:制备的发光玻璃中出现基质组分的结构特征峰及Dy~(3+)的能级跃迁特征峰。在350 nm波长光激发下,样品的发光强度、黄蓝发射峰比、荧光寿命、色坐标及色温等均随Dy~(3+)浓度的变化发生明显的可调节变化。样品的荧光发射强度随Dy~(3+)浓度的增加呈现先增大后减小的变化,当Dy~(3+)掺杂摩尔分数为1.0%时,发光强度最大。此外,随着Dy~(3+)掺杂浓度的增大,发光玻璃的荧光寿命及发射光谱的色度坐标值、色温都呈现递减的趋势。这表明通过基质组分及掺杂元素的调节可以使得该硼酸盐体系发光玻璃获得高效可调节的光功能从而得到广泛应用。     

与掺杂浓度相关的ZnS∶Mn纳米粒子的发光性质

采用溶胶法制备了Mn掺杂的ZnS纳米粒子,探讨了掺杂离子浓度对ZnS∶Mn纳米粒子的晶体结构和发光性质的影响。通过X射线衍射（XRD）对样品的结构进行了表征,结果表明：所制备的ZnS∶Mn纳米粒子为立方闪锌矿结构,其在Mn离子的掺杂浓度达到6%时不发生分相,但随着掺杂浓度的增加,纳米粒子的平均粒径会减小。光致发光光谱和荧光光谱的结果表明：通过改变掺杂离子的浓度可实现对ZnS∶Mn纳米粒子590 nm附近荧光发射波长的调节。此外,研究了温度对纳米粒子形貌和发光性质的影响。高分辨透射电子显微镜（HRTEM）观察发现,经过50℃陈化1 h后的ZnS∶Mn样品的平均粒径增大约为20 nm,且加热陈化有利于ZnS∶Mn纳米粒子中Mn2＋在590 nm处产生荧光。     

AE的分布及其在ZnO NPs作用下的颜色与光谱分析

氧化锌纳米粒子(ZnO NPs)是应用非常广泛的一种多功能无机材料,主要应用于化妆品、涂料、抗菌等领域。ZnO纳米粒子的大量使用增加了与生物接触的机会,可能会对生态环境产生一定的影响。芦荟是百合科常绿多肉质草本植物,具有重要的观赏和药用价值。芦荟大黄素(Aloe-emodin, AE)是芦荟中重要的色素分子,也是芦荟作为药用植物的重要有效成分。因此,以芦荟为实验对象,利用荧光显微镜通过纵向切片的方法观察了AE在叶片中的分布,较横向切片法更为全面、清晰地揭示了AE在叶片中的分布情况。通过荧光光谱结合颜色变化研究了ZnO纳米粒子与AE的相互作用。结果表明,在黑暗条件下,ZnO纳米粒子处理后溶液颜色由淡黄色逐渐变成橙色;紫外光照射使得AE溶液颜色变化加快,在相同的作用时间内,溶液颜色变得更深,由淡黄色逐渐变成橙红色。光谱研究发现,AE的荧光光谱有四个发光峰,分别是500,540,580与630 nm,与对照组相比,ZnO纳米粒子引起芦荟大黄素540和580 nm两个荧光峰的相对强度发生变化,随着ZnO纳米粒子作用时间的增加,I₅₄₀/I₅₈₀比值逐渐增大。     

饱和激发下叶绿素荧光非线性变化及影响分析

叶绿素浓度是海洋初级生产力的重要指标之一,激光诱导荧光技术可以实现海水叶绿素浓度的快速测量。测量叶绿素浓度的传统激光诱导荧光原理,是利用叶绿素荧光与水体Raman散射的强度比值（I_F/R）进行反演,即叶绿素浓度n_chl＝CI_F/R,其中C为系统常量。这是依据叶绿素荧光685 nm、水体Raman散射强度都与激发光强呈线性关系。然而,该理论并没有考虑诱导荧光饱和现象的存在。当诱导激光强度达到一定程度后,685 nm荧光强度随激发光强非线性变化。另外,值得注意的是,水体Raman散射并不存在信号饱和现象。为了探讨饱和激发造成荧光非线性变化的影响,在激光诱导荧光技术测量叶绿素浓度的实验中,设计两种测量方案,即：不同激光功率诱导单一浓度样本的荧光测量,和固定激光功率时不同浓度样本的荧光测量。实验中利用Nd∶YAG三倍频激光355 nm激发获得叶绿素溶液的404 nm处 Raman散射和685 nm荧光。实验结果分为2部分进行讨论：（1）为了分析饱和激发造成荧光变化的非线性特性,通过调节激发光功率测量溶液的受激发射光谱,发现水体Raman散射强度与激发光强呈线性关系,而685 nm荧光强度出现饱和激发下的非线性变化。而且,随叶绿素浓度的增加,685 nm荧光的非线性趋势更为明显,Raman散射强度与激发光强的线性关系中斜率变小。数据分析表明,685 nm荧光数据拟合的4阶多项式和Raman散射效率值,可以定性地表征685 nm荧光的饱和程度。（2）考虑实际海洋激光雷达探测叶绿素浓度应用中存在饱和激发荧光非线性现象,为了分析荧光非线性对传统叶绿素浓度反演理论适用性的影响,在固定激发光强情况下对不同浓度叶绿素溶液的发射光谱进行测量。将激发光功率调节至52.00,80.70,132.10和197.30 mW·cm-2,获取相应激发光强下685 nm荧光与水体Raman散射的强度比值和叶绿素浓度之间的关系。实验表明,激发光强不变的情况下,685 nm荧光与水体Raman散射的强度比值,与叶绿素浓度仍满足线性关系。但是,在较高光强激发时,饱和激发造成的叶绿素荧光非线性变化,导致利用传统激光诱导荧光理论反演的叶绿素浓度值偏小。因此,需要对饱和激发下荧光非线性的影响进行修正,其关系为I_F/R=n_chl/C+C_F,修正值C_F不可忽略。另外,值得一提的是,修正关系中系统常量C随激发光强增加而增大。研究表明,饱和激发造成的荧光非线性,会对激光诱导荧光技术测量叶绿素浓度产生影响,但由于造成荧光非线性因素的复杂性,仅通过荧光数据拟合获得的多项式,无法定量说明其影响权重。然而,当激发光强不变时,可以实验测量获得基于激光诱导荧光原理的修正关系,从而准确反演叶绿素浓度。     

Mn/PbTe(111)界面行为的光电子能谱研究

利用X光电子能谱(XPS)对Mn在PbTe(111)表面上沉积生长的界面性质进行了研究.研究表明Mn的沉积使衬底发生了原子尺度上的突变及金属/半导体界面的形成.从X光电子能谱的芯态能级峰来看,随着Mn膜的沉积Pb 4f峰的低结合能端出现了金属Pb的特征新峰,而Te 3d峰的高结合能端却出现了MnTe特征新峰.且随着Mn膜厚度的增加这些新峰变得越来越明显,当Mn膜厚度超过7 ML(monolayer)(即超过Pb,Te的探测深度)时,衬底信号峰完全消失,只剩下金属Pb和MnTe的芯态能级峰.Mn膜厚度继续增 关键词： PbTe半导体 界面形成 光电子能谱 偏析     

荧光光谱检测的酸性橙Ⅱ的研究

酸性橙Ⅱ在食品工业中是禁用添加剂.针对酸性橙Ⅱ的食品安全检测问题,报道了运用荧光光谱技术检测其水溶液的实验.实验表明,酸性橙Ⅱ水溶液在230～290nm波长激发下,310～390nm范围内产生荧光光谱,峰位波长在350nm,最佳激励波长为250nm;采用垂直偏振片(起偏角为0°)起偏照射样品,发现偏振荧光峰位不变,荧光峰强度随检偏角的增大而呈明显的线性递减关系.由实验数据计算得到荧光偏振度为0.783,表明分子具有一定确定取向;另外,分析认为酸性橙Ⅱ产生荧光,是由于分子中含有苯环和萘环结构吸收紫外光能量,以及氮键在光子作用下形成顺式异构体的激发单线态后,两者发射的光子所致.整个结果对酸性橙Ⅱ在食品中的违禁使用检测、特性表征、以及分子规律的更深入研究,有一定的参考价值.     

Determination of the Constants of Binding of Acridine Dyes with Micelles of Sodium Dodecyl Sulfate Using the Quenching of Delayed Fluorescence by Heavy Atoms

The constants of binding dye molecules with the micelles of sodium dodecyl sulfate are determined using quenching of delayed fluorescence of acridine dyes by sodium iodide in aqueous–micellar solutions. Kinetic equations have been composed that describe the processes of deactivation of the excited states of dyes. By solving these equations at the concentration of the quencher sodium iodide corresponding to the minimum lifetime of triplet states and at the concentration of micelles corresponding to the least value of the delayed fluorescence quenching rate constants, we obtained the constants of binding dyes with micelles equal to 1.3·10⁷, 2.9·10⁷, and 3.1·10⁷ M^–1 for trypaflavine, acridine orange, and acridine yellow, respectively. We calculated the rate constants of quenching of the triplet states of the molecules of dyes by iodide ions (I ^–) that decreased in transition from trypaflavine to acridine orange and acridine yellow.     

UV induced photoluminescence and thermally stimulated luminescence of ThO2:Tb3+ phosphor

Thorium oxide doped with trivalent terbium ions offers itself as a novel phosphor with its photo- and thermally-stimulated luminescence (PL and TSL) characteristics showing a marked change on sustained exposure to 254 and 365 nm ultraviolet (UV) radiation. The reduction in luminescence intensity of Tb³⁺ ions, on irradiation with 254 nm photons and subsequent restoration on exposure to 365 nm, has been correlated with the complimentary behaviour in UV-induced TSL. These changes are, in turn, ascribed to inter-configurational (f–d) transitions and e–h formation and recombination processes. UV radiation induced TSL output increases linearly with incident UV radiant energy at a constant radiation flux; however, for a fixed exposure, TSL output increases with increase in radiant flux.