Sm3+/Ce3+/Tb3+共掺CaO-B2O3-SiO2发光玻璃的制备及发光性能研究

采用高温熔融法制备了Sm3+/Ce3+/Tb3+共掺杂的CaO-B2O3-SiO2发光玻璃材料,并用荧光分光光度计和CIE色度坐标对其发光性能进行了研究。发射光谱表明,在374nm激发下,Sm3+/Ce3+/Tb3+共掺杂CaO-B2O3-SiO2发光玻璃的发射光谱中同时观测到了红橙光、蓝光和绿光的发射带,这些发射带的混合实现了白光发射。此外,在Sm2O3和Tb4O7含量不变的情况下,随着CeO2含量的减小,Sm3+/Ce3+/Tb3+共掺杂发光玻璃的发光颜色在白光区逐渐由蓝光区附近过渡到黄光区附近。     

Eu2+在KNaCa2（PO4）2中的发光及晶体学格位

采用高温固相法制备了KNaCa2(PO4)2:Eu2+蓝色荧光粉,并研究了材料的发光特性.在400 nm近紫外光激发下,材料呈非对称的单峰发射,主峰位于470 nm.监测470 nm发射峰,对应的激发光谱覆盖200~450 nm,主峰位于400 nm,说明材料能够很好的吸收紫外?近紫外光,发射蓝色光.利用van Uitert公式计算了Eu2+取代KNaCa2(PO4)2中Ca2+时所占晶体学格位,得出461和502 nm发射分别归属于八配位和六配位的Eu2+发射.研究了Eu2+掺杂浓度对KNaCa2(PO4)2:Eu2+材料发射强度的影响,结果显示Eu2+的最佳掺杂浓度为1mol%,利用Dexter理论得出其浓度猝灭机理为电偶极?电偶极相互作用.     

白光LED用KNaCa2（PO4）2∶Dy3+材料的制备与发光特性研究

采用高温固相法制备了KNaCa2(PO4)2∶Dy3+发光材料并对其发光特性进行了研究。光谱显示,KNaCa2(PO4)2∶Dy3+激发谱为300～500nm范围内的一系列锐谱,可被InGaN管芯和蓝光有效激发。尤其在385nm紫外光激发下,样品呈现较强白光发射,主发射峰位于485和577nm,对应Dy3+的4F9/2-6 H15/2、4F9/2-6 H13/2跃迁,形成"黄+蓝"单一基质白光。研究了Dy3+掺杂浓度对KNaCa2(PO4)2∶Dy3+发光性能的影响,随Dy3+浓度增加,发光强度先增大后减小,最佳掺杂浓度为0.04mol,Y/B值在较小范围内先增大后减小。根据Dexter理论分析其浓度猝灭机理为电偶极-电偶极相互作用。测量并标定了Dy3+不同浓度下样品的色坐标均呈现白光发射。研究表明,KNaCa2(PO4)2∶Dy3+材料是一种适合紫外-近紫外-蓝光激发的单一基质白光荧光粉。     

Eu2+离子在Sr2Al6O11基磷光体中发光行为的研究

研究了不同Eu掺杂浓度对Sr2Al6O11基磷光体发光性能的影响。结果发现，当Eu掺杂浓度低于0.01mol时，在其发射光谱中存在403和493nm的主发射峰，对应着Sr2Al6O11基质中Sr的两种不同位置Sr1和Sr2位。随着Eu掺杂浓度增加，由于能量传递作用，导致403nm的发射峰消失，493nm的发射峰增强。余辉衰减曲线表明，未掺杂Dy的磷光体没有余辉性能，当Eu掺杂量在0.01mol时，余辉性能最好，进一步提高Eu的掺杂量，由于浓度猝灭作用，导致发光性能下降。     

白光LED用新型红色荧光粉Sr5（BO3）3Cl:Eu3+的制备与发光特性

采用高温固相法合成了Sr5(BO3)3Cl:Eu3+新型红色发光材料,并对其结构和发光特性进行了研究。X射线衍射测试表明合成材料为纯相Sr5(BO3)3Cl晶体。材料的主发射峰位于587,596,613nm和626nm,对应Eu3+的5 D0→7F1,7F2辐射跃迁。监测626nm发射峰,激发光谱主峰位于392nm,可被InGaN管芯有效激发。通过时间分辨光谱测得Eu3+离子5 D0能级的荧光寿命约为2.28ms。研究了Eu3+离子掺杂浓度对Sr5(BO3)3Cl:Eu3+发光性能的影响,结果随着Eu3+离子浓度的增大,样品的发光强度先增大后减小,最佳掺杂浓度为16%(摩尔分数)。计算了Eu3+离子浓度猝灭的临界距离为1.46nm。测量了不同Eu3+浓度样品的色坐标,均位于色品图红光区,符合NTSC标准。     

Eu^3＋掺杂浓度对LaInO3∶Eu^3＋红色荧光粉发光性能影响及自身猝灭机理研究

采用高温固相反应法合成了新型LaInO3∶Eu3＋红色荧光粉。晶体物相和发光性能分别用XRD、荧光分度计进行表征。XRD图谱表明在1150℃制备了纯相的LaInO3∶Eu3＋荧光粉。该荧光粉能够被394nm近紫外光和464nm蓝光有效激发,其最强发射峰位于610nm处,对应于Eu3＋离子的5 D0→7F2的特征发射。改变Eu3＋离子掺杂浓度,发射峰形状和位置基本不变,发射强度在Eu3＋离子浓度超过20%（摩尔分数）时剧烈下降,出现了浓度猝灭效应。Eu3＋位于610nm的发射自身猝灭机理是电四极-电四极的相互作用。研究结果显示LaInO3∶Eu3＋是一种有潜力的用于制造白光LED的红色荧光粉。     

白光LED用钨酸盐红色荧光粉的制备及发光特性

采用高温固相法制备了NaY(WO4)2:Eu3+发光材料。分别用X射线粉末衍射(XRD)、发光光谱(PL)等手段研究了发光粉的晶体结构以及发光性能。XRD结果表明,Eu3+掺杂浓度达到25%(摩尔分数)时,仍然能够形成纯相的NaY(WO4)2:Eu3+多晶粉末。NaY(WO4)2:Eu3+的激发光谱由强度很大的宽激发带(220～300nm)和锐线谱(峰值位于393nm和465nm)组成,其中宽激发带源于O2-→W6+和O2-→Eu3+电荷转移,锐线谱属于Eu3+的4f-4f跃迁吸收,发射光谱显示随Eu3+浓度的增大,NaY(WO42):Eu3+光发射强度逐渐增大,当Eu3+浓度为20%时,发射强度达到最大,随后出现浓度猝灭。     

Ce3+、Mn2+掺杂Zn3（BO3）2的制备及其发光性能

采用共沉淀法在700℃和较短的烧结时间下制备了Zn3(BO3)2和不同浓度的Ce3+、Mn2+离子掺杂的Zn3(BO3)2纳米晶粉末,对合成产物的发光性质及发光机理进行了研究。利用荧光分光光度计、X射线粉末衍射仪以及透射电镜对其光学性能和纳米晶形貌进行了表征。结果表明Ce3+离子掺杂的Zn3(BO3)2样品在340～400nm之间有强的荧光发射,其最高发射峰峰位为365nm,在Ce3+掺量为0.5%(摩尔分数,下同)时发光强度达到最高值。Ce3+取代Zn2+离子作为发光中心,Mn2+离子作为激活剂加入,并不影响荧光发射峰的位置,但能够有效增强其发光强度。当Mn2+离子掺量为0.7%(摩尔分数)时,Ce3+、Mn2+共掺杂的Zn3(BO3)2纳米晶发光强度达到最高值。     

紫外激发蓝色荧光粉Sr2-x-yB5O9Cl:xEu2+,yTb3+的合成和发光性能

采用高温固相反应法合成Sr_2-x-yB₅O₉Cl:xEu²⁺,yTb³⁺蓝色荧光粉。用X射线衍射表征材料的晶体结构、用荧光光谱仪测定Eu²⁺和Tb³⁺的掺杂浓度,研究了助溶剂H₃BO₃过量浓度和反应温度对荧光粉发光性质的影响。结果表明,单掺杂Eu²⁺时,其浓度猝灭机理为电偶极-电偶极交互作用机制,浓度猝灭临界距离为R_C=1.71 nm。在紫外（230-410 nm）波段有强而宽的吸收带,表明此粉是一种近紫外白光LED用的蓝色荧光粉。     

Eu3+掺杂的钼酸盐微纳米材料制备和光致发光性能研究

分别采用沉淀法和水热法成功制备了Y_2(MoO_4)_3∶Eu~(3+)红色荧光粉,使用X射线粉末衍射(XRD)、扫描电子显微镜(SEM)和荧光光谱对其物相结构、形貌和发光性能进行表征。结果表明:Eu~(3+)含量低于20%(摩尔分数,下同)不会改变Y_2(MoO_4)_3的晶体结构;沉淀法得到荧光粉呈花状,而水热法主要得到层层堆积结构的荧光粉;所制荧光粉的主激发峰和发射峰分别位于394和614nm,这是来自掺杂Eu~(3+)的f-f电子跃迁。Y_2(MoO_4)_3荧光粉中Eu~(3+)最佳摩尔分数为20%,当Eu~(3+)含量大于20%时,出现浓度猝灭现象,其5D_0→7F_2发光浓度猝灭机理是电偶极-电偶极相互作用。     

Eu2+、Dy3+、Li+共掺杂CaSi2O2N2荧光粉的发光性能

采用高温固相反应法制备了一系列白光LED用CaSi2O2N2:0.05Eu2+,xDy3+,xLi+(0≤x≤0.03)荧光粉.利用X射线衍射仪对样品的物相结构进行了分析,结果表明:Dy3+和Li+离子的掺入没有改变CaSi2O2N2:Eu2+荧光粉的主晶相.利用荧光光谱仪对样品的发光性能进行了测试,发现所有样品的激发光谱均覆盖了从近紫外到蓝光的较宽范围,400 nm激发下得到的发射光谱为宽波段的单峰,峰值位于545 nm左右,是Eu2+离子5d-4f电子跃迁引起的.Dy3+离子掺杂可以提高CaSi2O2N2:Eu2+荧光粉的发光强度,Dy3+与Li+共掺杂可进一步提高荧光粉的发光强度,当Dy3+和Li+的掺杂量为1mol%时,荧光粉的发光强度达到最大值,是单掺杂Eu2+的荧光粉发光强度的157%.     

Template-free Fabrication and Luminescent Characterization of Highly Uniform and Monodisperse Y2O2S:Sm3+ Hollow Submicrospheres

Well dispersed and homogeneous Y2O2S:Sm3+ hollow submicrospheres were successfully achieved by a templatefree solvothermal method combining with a postcalcining process.The crystalstructure and particle morphology were investigated by the X-ray diffraction(XRD),Fourier transform infrared(FT-IR) spectra,scanning and transmission electron microscopy(SEM and TEM),respectively.A possible growth mechanism was proposed to reveal the formation process.Luminescence properties of the Y2O2S:Sm3+ long-lasting phosphor were analyzed by measuring the excitation spectra,emission spectra,afterglow decay curve and thermoluminescence curve.The excitation spectra indicated that the phosphor could be excited effectively by the ultraviolet-light emitting diode(UV-LED) or blue LED,and the emission spectra showed that the phosphor could emit red light from 600 to 650 nm.     

Sol-gel fabrication and photoluminescence properties of SiO2 @ Gd2O3:Eu3+ core-shell particles

A uniform nanolayer of europium-doped Gd2O3 was coated on the surface of preformed submicron silica spheres by a Pechini sol-gel process. The resulted SiO2 @ Gd2O3:Eu3+ core-shell structured phosphors were characterized by X-ray diffraction (XRD), Fourier transform infrared spectroscopy (FT-IR), field emission scanning electron microscopy (FESEM), transmission electron microscopy (TEM), photoluminescence (PL) spectra as well as kinetic decays. The XRD results show that the Gd2O3:Eu3+ layers start to crystallize on the SiO2 spheres after annealing at 400 degrees C and the crystallinity increases with raising the annealing temperature. The core-shell phosphors possess perfect spherical shape with narrow size distribution (average size: 640 nm) and non-agglomeration. The thickness of the Gd2O3:Eu3+ shells on the SiO2 cores can be adjusted by changing the deposition cycles (70 nm for three deposition cycles). Under short UV excitation, the obtained SiO2@Gd2O3:Eu3+ particles show a strong red emission with 5D0-7F2 (610 nm) of Eu3+ as the most prominent group. The PL intensity of Eu3+ increases with increasing the annealing temperature and the number of coating cycles.     

Characterization and luminescence of Eu3+ ions doped 12CaO 7Al2O3 nanopowders

Eu3+ ions doped 12CaO 7Al2O3 (C12A7) powders with different Eu3+ concentrations were prepared by sol-gel combined with solid state reaction method. The results of XRD and Raman spectra showed that single cubic phase polycrystalline C12A7:Eu3+ powders were prepared. The absorption peaks attributed to f-f transition of Eu3+ ion can be observed, indicating that Eu3+ had been incorporated into C12A7 lattice site. Visible PL peaks around 578, 588, 614 nm were ascribed to 5D0 --> 7FJ (J = 0, 1, 2) transitions of Eu3+ under the excitation of 488 nm line. The PL of C12A7:Eu3+ showed the strongest emission intensity at Eu3+ concentration of 0.5 at%. Two different types of Eu3+ centers were identified by the two lines from 5D0 --> 7F0 transition emission. The doping mechanism of C12A7:Eu3+ might be attributed to Eu3+ ions substitution for two types of Ca2+ lattice sites in C12A7. The temperature dependent PL spectra of Eu-doped C12A7 were measured in the range from 100 to 300 K under the excitation of 488 nm laser line. The PL intensities as a function of temperature were well fitted by using a unified theoretical model, considering thermal activation and nonradiative energy transfer processes.     

Luminescence properties of nano-crystalline Ba3MgSi2O8:Eu2+, Mn2+ phosphors

Ba3MgSi2O8:Eu2+, Mn2+ phosphors were synthesized by the sol-gel method and high temperature solid-state reaction method, respectively. XRD (X-ray diffraction), FT-IR (Fourier transform infrared spectroscopy), PL (photoluminescence spectra), and PLE (photoluminescence excitation spectra) were measured to characterize the samples. Emission and excitation spectra of our Ba3MgSi2O8:Eu2+, Mn2+ phosphors monitored at 441, 515, and 614 nm are depicted in the paper. The emission intensities of 441 and 515 nm emission bands increase with increasing Eu2+ concentration, while the peak intensity of the 614 nm band increases with increasing Mn2+ concentration. We conclude that the 515 nm emission band is attributed to the 4f(6)5d transition of Eu2+ ions substituted by Ba2+ sites in Ba2SiO4. The 441 nm emission band originates from Eu2+ ions, while the 614 nm emission band originates from Mn2+ ions of Ba3MgSi2O8:Eu2+, Mn2+. Nano-crystalline Ba3MgSi2O8:Eu2+, Mn2+ phosphors prepared by the sol-gel method show higher color rendering and better color temperature in comparison with the samples prepared by high temperature solid-state reaction method.     

Synthesis and luminescence properties of Sr2SiO4: Eu3+, Dy3+ phosphors by the sol-gel method

The Sr2SiO4:Eu3+, Dy3+ phosphors for white light emitting diodes (LEDs) were synthesized by the sol-gel method. The microstructure and luminescent properties of the obtained Sr2SiO4:Eu3+, Dy3+ particles were well characterized. The results demonstrate that the Sr2SiO4:Eu3+, Dy3+ particles, which have spherical morphology, emitted an intensive white light emission under excitation at 386 nm. The phosphors show three emission peaks: the blue emission at 486 nm corresponding to the 4F(9/2)-6H(15/2) transition of Dy3+, the yellow emission at 575 nm corresponding to the 4F(9/2)-6H(13/2) transition of Dy3+, and the red emission at 615 nm corresponding to the 5D0-7F2 transition of Eu3+. At the same time, the effect of Eu3+ concentration on the emission intensities of Sr2SiO4:Eu3+, Dy3+ was investigated in detail. The phosphors used for white LEDs were obtained by combining near ultraviolet (NUV) light (386 nm) with Sr2SiO4:0.04Dy3+, 0.01Eu3+ phosphors with the characteristic of Commission Internationale de l'Eclairage (CIE) chromaticity coordinate (x, y) of (0.33, 0.34), and color temperature Tc of 5,603 K. In addition, the effect of the charge compensators (Li+, Na+, and K+ ions) on the photoluminescence (PL) emission intensities were studied.     

Effect of concentration on the photoluminescence properties of Sm3+ and Dy3+: cadmium lithium boro tellurite glasses

Rare-earth (Sm3+ or Dy3+) ions doped cadmium lithium boro tellurite glasses have been prepared by melt quenching method for their spectral studies. From X-ray diffraction (XRD) patterns the glass amorphous nature has been confirmed. Vis-NIR absorption, excitation and emission spectra of these glasses have been analyzed systematically and also rare earth ion concentration is optimised Sm3+: CLiBT glasses have shown strong orange-reddish emission at 598 nm (4G5/2-->6H7/2) with an excitation wavelength lambda(exci) = 401 nm and Dy3+: CLiBT glasses have shown strong yellow emission at 574 nm (6F9/2-->6H13/2) with lambda(exci) = 451 nm.     

Emission Properties of Yb3+/Er3+ Doped TeO2-WO3-ZnO Glasses for Broadband Optical Amplifiers

The YbS /Er3 doped TeO2-WO3-ZnO glasses were prepared. The absorption spectra, emission spectra and fluorescence lifetime of Era at 1.5μm, excited by 970 nm were measured. The influence of Er2Oa, Yb2Oa and Ohcontents on emission properties of Era at 1.5 μm was investigated. The optimum doping concentrations for Era and Yba is around 3.34× 1020 ions/cma and 6.63×1020 ions/cma, respectively. The peak emission cross section is 0.83～0.87 pm2. With the increasing concentration of Yba , the FWHM of Era emission at 1.5 μm in the glass increases from 77 nm to 83 nm. The results show that Yba /Era doped meO2-Woa-ZnO glasses are promising candidate for Era -doped broadband optical amplifier.     

Ce3+掺杂Li2O-MgO-Al2O3-SiO2玻璃的结构与荧光猝灭现象

采用熔融淬冷法制备了不同浓度Ce³⁺离子掺杂的20Li₂O-5MgO-20Al₂O₃-55SiO₂玻璃闪烁材料。采用X射线衍射(XRD)、高分辨透射电镜(HRTEM)技术、密度检测等方法研究了玻璃的微观结构随Ce³⁺离子掺杂浓度的变化规律, 采用荧光分光技术检测了玻璃的紫外光致激发光谱(PLE)、发射光谱(PE)。研究结果表明: 在不对称的晶体场作用下, Ce³⁺离子5d能级被劈裂为5个组分; 随着玻璃基质内Ce³⁺离子掺杂浓度增大, 玻璃的非晶化程度加深; 5d能级的劈裂宽度随之增大, 由此导致激发带向低能量端展宽、发射光谱明显红移; Ce³⁺离子的荧光发射强度随Ce³⁺离子掺杂浓度先升高、后降低, 浓度猝灭过程成为其荧光发射效率降低的主要原因。