近紫外光激发黄色荧光粉Ba3Y4O9：Dy3+的制备及发光特性

通过高温固相法合成了一系列Ba₃Y_4-xO₉：xDy³⁺荧光粉材料。利用X射线粉末衍射、荧光光谱和荧光寿命对样品进行了表征。实验表明,样品的激发光谱由一系列线状峰组成,峰值分别位于328,355,368,386,427,456,471 nm。在355 nm激发下,荧光粉在490 nm（⁴F_9/2→⁶H_15/2）和580 nm（⁴F_9/2→⁶H_13/2）处有很强的发射,发射光谱的色坐标位于黄光区域。研究了不同Dy³⁺掺杂浓度对样品发光性质的影响,发现样品的发光随着Dy³⁺浓度的增大而增强,但光谱形状基本保持不变,表明Dy³⁺占据了基质中低对称性的Y³⁺格位。当Dy³⁺摩尔分数x=0.08时出现发光强度猝灭现象,浓度猝灭机理为电偶极-电偶极相互作用。样品的发光寿命随着Dy³⁺浓度的增大逐渐减小,进一步证明了Dy³⁺离子之间存在着能量传递现象。Ba₃Y₄O₉：Dy³⁺荧光粉的发光位于黄光区域,有较好的热稳定性,是潜在的白光LED用荧光粉材料。     

纳米棒状GdPO4:Eu3+荧光粉的合成及其发光性能的研究

采用溶解热法合成出了纳米棒状GdPO₄:Eu³⁺荧光粉,其中不同磷源和pH值对最终产物的形成起着关键的作用. 将纳米棒状和块体GdPO₄:Eu³⁺荧光粉的发光性能进行了对比,其中与块体GdPO₄:Eu³⁺荧光粉相比,纳米棒状GdPO₄:Eu³⁺荧光粉的色纯度得到了改善,而在激发光谱中,纳米棒状GdPO₄:Eu< 关键词： 纳米棒 磷酸钆 发光性能     

白光LED用Ca3Si3O9：Dy3+荧光粉的制备及其发光性能

采用溶胶-凝胶法制备了可用于白光LED的新型Ca₃Si₃O₉:Dy³⁺荧光粉, 通过对样品的X 射线衍射谱及光致发光光谱的测试和表征, 研究了Ca₃Si₃O₉:Dy³⁺的物相结构和发光性能. 结果显示, Ca₃Si₃O₉:Dy³⁺的发射光谱是由位于483 nm和577 nm处的主峰构成的双峰谱线, 激发光谱为多峰宽谱, 谱峰位于290–480 nm范围内. Dy³⁺掺杂浓度对Ca₃Si₃O₉:Dy³⁺发光性能有明显的影响, 随着Dy³⁺浓度的增大, Ca₃Si₃O₉:Dy³⁺的发光强度和黄、蓝光发射强度比 (Y/B) 均呈现先增大后减小的规律, 最大发光强度值对应的Dy³⁺浓度为1 mol%. 电荷补偿剂Li⁺能提高Ca₃Si₃O₉:Dy³⁺的发光强度, 特别当Li⁺浓度为2–4 mol%时, 荧光粉的蓝光发射强度显著增大. 关键词： 白光LED 溶胶-凝胶法 3Si₃O₉：Dy³⁺')" href="#">Ca₃Si₃O₉：Dy³⁺ 发光特性     

La7（1-x）P3O18:xDy3+的白光发光性能

使用高温固相法制备了La_7（1-x）P₃O₁₈:xDy³⁺发光材料,在347nm激发下,其发射峰分别为480、578、664nm,分别对应离子Dy³⁺能级内的⁴F_9/2→⁶H_15/2、⁶H_13/2和⁶H_11/2跃迁。随着Dy³⁺浓度的增加,黄光和蓝光的强度的比值逐渐减小,当Dy³⁺浓度为2mol%时,发光强度最大,计算出的色坐标处于白光区域内（0.33,0.33）,该材料的发光颜色随Dy³⁺浓度的变化而在白光区域内改变,因此,该材料可作为紫外激发的白色发光材料。     

掺稀土元素Dy和Mn,P,Cu的MgSO4的热释发光光谱

实验测定了MgSO₄:Dy,Mn和MgSO₄:Dy,P以及MgSO₄:Dy,P ,Cu等的热释光磷光体的三维发光谱.结果表明,掺入Dy的MgSO₄磷光体的热释发 光谱线的波长与Dy³⁺离子的能级跃迁相关,Dy³⁺为热释光主要发光 中心.MgSO₄中只掺入Mn时,温度在140℃和190℃附近呈现波长为660nm宽范围的 连续发光带,这是Mn形成的发光中心的 关键词： 热释发光光谱 稀土元素镝 硫酸镁     

中子探测晶体Li6Gd(BO3)3:Ce的光谱特性研究

文章用提拉法生长出Li₆Gd(BO₃)₃:Ce晶体,并对其光谱性能与发光过程进行了探索. 借助于真空紫外-紫外透过光谱测试,发现晶体的透过光谱中存在Ce³⁺离子和Gd³⁺的特征吸收峰,同时还存在与Ce⁴⁺离子相关的电荷迁移带. 对晶体的真空紫外-紫外激发发射光谱进行研究发现,在晶体存在着Ce³⁺离子的5d→4f辐射跃迁发光与Gd³⁺离子的4f→4f辐射跃迁发光,而且存在着Gd³⁺→Ce³⁺之间的能量传递. 对Li₆Gd(BO₃)₃:Ce晶体的X射线与γ射线激发发射光谱研究可知,晶体在高能射线激发下的闪烁光主要是Ce³⁺离子的发光. 关键词： 6Gd(BO₃)₃:Ce晶体')" href="#">Li₆Gd(BO₃)₃:Ce晶体 真空紫外-紫外透过光谱 真空紫外-紫外激发发射光谱 能量传递     

Ca2SiO4:Dy3+材料的制备及其发光特性

采用高温固相法制备了Ca₂SiO₄:Dy³⁺发光材料.在365nm紫外光激发下,测得Ca₂SiO₄:Dy³⁺材料的发射光谱为一多峰宽谱,主峰分别位于486nm,575nm和665nm处;监测575nm发射峰,测得材料的激发光谱为一多峰宽谱,主峰分别位于331nm,361nm,371nm,397nm,435nm,461nm和478nm处.研究了Dy³⁺掺杂浓度对Ca₂SiO₄:Dy³⁺材料发射光谱及发光强度的影响,结果显示,随Dy³⁺浓度的增大,黄、蓝发射峰强度比(Y/B)逐渐增大,利用Judd-Ofelt理论解释了其原因;随Dy³⁺浓度的增大,Ca₂SiO₄:Dy³⁺材料发光强度先增大,在Dy³⁺浓度为4 mol%时到达峰值,而后减小,根据Dexter理论其浓度猝灭机理为电偶极-电偶极相互作用.研究了电荷补偿剂Li⁺,Na⁺和K⁺对Ca₂SiO₄:Dy³⁺材料发射光谱的影响,结果显示,不同电荷补偿剂下,随电荷补偿剂掺杂浓度的增大,Ca₂SiO₄:Dy³⁺材料发射光谱强度的演化趋势相同,即Ca₂SiO₄:Dy³⁺材料发射峰强度先增大后减小,但不同电荷补偿剂下,材料发射峰强度最大处对应的补偿剂浓度不同,对应Li⁺,Na⁺和K⁺时,浓度分别为4mol%,4mol%和3mol%. 关键词： 白光LED 2SiO₄:Dy³⁺')" href="#">Ca₂SiO₄:Dy³⁺ 发光特性 电荷补偿     

稀土掺杂Gd2Te4O11亚碲酸盐荧光粉的合成及其发光性能

采用水热法制备了一系列稀土Dy³⁺,Tb³⁺,Eu³⁺掺杂的极性Gd₂Te₄O₁₁(GTO)亚碲酸盐荧光粉.对样品的物相结构、形貌和热稳定性等进行了表征,测试了样品的发光性能.结果显示,所制样品均为单相,呈短杆状形貌,尺寸在微米量级,热稳定性能良好.对于GTO:Dy³⁺荧光粉,在紫外光激发下的发光主要位于黄绿光区,获得最强发光强度的掺杂浓度为2.5%,色坐标为(0.39,0.43);荧光衰减曲线表明GTO:Dy³⁺样品发光寿命随着掺杂浓度增大逐渐减小,与Dy³⁺离子间的交叉弛豫有关.对于GTO:Eu³⁺荧光粉,在紫外光激发下的发光主要位于红光和橙红光区,其发射强度随着Eu³⁺掺杂浓度的增大而增强.当掺杂浓度为10%时,样品发光的色坐标为(0.62,0.38),位于橙红光区,且样品的发光寿命几乎不受掺杂浓度影响.对于GTO:Tb³⁺     

蓝色长余辉材料Sr2MgSi2O7：Eu2+,Dy3+及其基质的VUV-UV激发特性

Sr₂MgSi₂O₇:Eu²⁺,Dy³⁺是一种有效的蓝色长余辉材料,采用高温固相法合成了Sr₂MgSi₂O₇,Sr₂MgSi₂O₇:Dy³⁺,Sr₂MgSi₂O₇:Eu²⁺及Sr₂MgSi₂O₇:Eu²⁺,Dy³⁺,利用同步辐射研究了它们的VUV-UV激发特性.在真空紫外光激发下,在基质中发现了稍弱的位于385nm的发射带,在双掺杂的样品中,除了Eu²⁺的4f5d→4f发射带(465nm)外,还观察到了575nm处的发射峰;通过和Dy³⁺单掺杂样品的发射谱比较,发现它是来自于Dy³⁺的4f-4f(⁴F_9/2→6H_13/2)跃迁.在它们的激发谱上可以看出Dy³⁺与基质发射的有效激发均处于真空紫外区,在近紫外及可见区激发下未见到它们发光.另外在Sr₂MgSi₂O₇:Eu²⁺,Dy³⁺中观察到Dy³⁺的发射也说明了Dy³⁺在该类长余辉材料中不仅作为陷阱用来延长余辉,而且也以发光中心形式存在于基质中.     

Dy3+掺杂NaYF4纳米粒子的制备及其上转换发光性质

制备了Dy³⁺掺杂 NaYF₄上转换发光纳米晶体,通过X射线衍射(XRD)、扫描电子显微镜(SEM)、荧光(FL)光谱、红外光谱仪(FT-IR)对合成样品的结构、形貌和发光性能进行表征。探讨了稀土离子掺杂浓度和焙烧温度对NaYF₄∶Dy³⁺纳米晶的结构、形貌和发光的影响。在776 nm红外光下激发样品,出现479,574 nm上转换发射峰,实现了蓝、绿上转换发光。绿光来自于Dy³⁺的⁴F_9/2→⁶H_13/2跃迁,蓝光是由Dy³⁺的⁴F_9/2→ ⁶H_15/2跃迁产生的。     

Dy3+ emission in M5(PO4)3F (M = Ca, Ba) phosphor

Ultrafine M₅(PO₄)₃F:Dy³⁺ (M = Ca, Ba) phosphors were prepared via combustion process using metal nitrates as precursors. The formation of crystalline phosphate was confirmed by X-ray diffraction pattern. The PL excitation spectra show the excitation peaks observed at 250 to 400 nm due to f → f transition of Dy³⁺ ion, which are useful for solid-state lighting purpose (mercury free excitation). The PL emission of Dy³⁺ ion by 348 nm excitation gave an emission at 489 nm (blue), 582 nm (yellow) and 675 nm (red). All the characteristics of BYR emissions like BGR indicate that Dy doped Ca₅(PO₄)₃F and Ba₅(PO₄)₃F phosphors are good candidates that can be applied in solid-state lighting phosphor (mercury free excited lamp phosphor) and white light LED.      

Luminescence of KCaSO4Cl:X, Y (X=Eu or Ce; Y=Dy or Mn) halosulfate material

Polycrystalline KCaSO₄Cl:Eu, Dy, KCaSO₄Cl:Ce, Dy and KCaSO₄Cl:Ce, Mn phosphors prepared by a solid state diffusion method have been studied for its photoluminescence (PL) characteristics. The presence of two overlapping bands at around 400 and 450 nm in the PL emission spectra of the phosphor suggests the presence of Eu²⁺ in the host compound occupying two different lattice sites. The effects of co-doping on the photoluminescence (PL) characteristics of KCaSO₄Cl:Eu or Ce phosphors have been studied. The decrease in peak intensity of the phosphor on co-doping it with Dy gives an insight into the emission mechanism of the phosphors, which involves energy transfer from Eu²⁺→Dy³⁺, Ce³⁺→Dy³⁺ and Ce³⁺→Mn²⁺.     

Photoluminescence and thermoluminescence characterization of Eu- and Dy -activated Ca3(PO4)2 phosphor

Rare-earth-doped polycrystalline Ca₃(PO₄)₂:Eu, Ca₃(PO₄)₂:Dy and Ca₃(PO₄)₂:Eu,Dy phosphors prepared by a modified solid-state synthesis has been studied for its X-ray diffraction, thermoluminescence (TL) and photoluminescence (PL) characteristics. The PL emission spectra of the phosphor suggest the presence of Eu³⁺ ion in Ca₃(PO₄)₂:Eu and Dy³⁺ ion in Ca₃(PO₄)₂:Dy lattice sites. The TL glow curve of the Ca₃(PO₄)₂:Eu compounds has a simple structure with a prominent peak at 228 °C, while Ca₃(PO₄)₂:Dy peaking at 146 and 230 °C. TL sensitivity of phosphors are compared with CaSO₄: Dy and found 1.52 and 1.20 times less in Ca₃(PO₄)₂:Eu and Ca₃(PO₄)₂:Dy phosphors, respectively. The Ca₃(PO₄)₂:Eu,Dy phosphors shows switching behavior under two different excitation wavelengths and enhancement in PL intensity of Dy³⁺ ions were reported. The paper discusses the photoluminescence and thermoluminescence behavior of Eu³⁺ and Dy³⁺ ion in Ca₃(PO₄)₂ hosts, it may be applicable to solid-state lighting as well as thermoluminescence dosimetry applications.     

Luminescence studies on SrMgAl10O17:Eu, Dy phosphor crystals

Using urea as fuel, SrMgAl₁₀O₁₇:Eu, Dy phosphor was prepared by a combustion method. Its luminescence properties under ultraviolet (UV) excitation were investigated. Pure SrMgAl₁₀O₁₇ phase was formed by urea-nitrate solution combustion synthesis at 550 °C. The results indicated that the emission spectra of SrMgAl₁₀O₁₇:Eu, Dy has one main peak at 460 nm and one shoulder peak near 516 nm, which are ascribed to two different types of luminescent Eu²⁺ centers existing in the SrMgAl₁₀O₁₇ matrix crystal. The blue luminescence emission of SrMgAl₁₀O₁₇:Eu phosphors was improved under UV excitation by codoping Dy³⁺ ions. The SrMgAl₁₀O₁₇:Eu phosphors showed green afterglow (λ=516 nm) when Dy³⁺ ions were doped. Dy³⁺ ions not only successfully play the role of sensitizer for energy transfer in the system, but also act as trap levels and capture the free holes in the spinel blocks.     

Synthesis and photoluminescence properties of NaPbB5O9:Dy phosphor materials for white light applications

Given the recent increased interest in phosphor materials and their applications, we analyzed a new NaPbB₅O₉:Dy³⁺ phosphor material with different concentrations of Dy³⁺. In particular, we investigated the crystal structure, morphology, and luminescence properties of these materials. X-ray diffraction analyses confirmed the formation of NaPbB₅O₉:Dy³⁺ phosphor powder. The functional groups present in the phosphor materials were examined by Fourier transform infrared spectroscopy. Scanning electron microscope images showed that the size of the grains was in the micrometer range. Photoluminescence spectra were recorded at different excitation wavelengths for the phosphor materials and we analyzed the variation in the intensity of the emission bands with different concentrations of Dy³⁺ ions. The color co-ordinates were calculated and used to characterize the color of the phosphor. We found that the emission colors of the Dy³⁺-doped NaPbB₅O₉ powders depended on the Dy³⁺ ion doping concentration and the excitation wavelength.     

Synthesis and optimum luminescence of monodispersed spheres for BaWO4-based green phosphors with doping of Tb

Monodispersed spheres for Tb³⁺-doped BaWO₄ (BWO:Tb) phosphors were prepared by a hydrothermal method. X-ray diffraction (XRD) and field-emission scanning electron microscopy were used to characterize the resulting samples. Emission and excitation spectra were studied using xenon excited spectroscopic experiments at room temperature. Because 12 at% BWO:Tb phosphor exhibits intensive green emission under 254 nm excitation in comparison with the commercial green fluorescent lamp phosphor (LaPO₄:Ce,Tb), it is considered to be a new promising green phosphor for fluorescent lamps application.     

Emission spectra of MgSO4:Dy,MgSO4:Tm and MgSO4:Dy,Mn phosphors

MgSO₄:Dy, MgSO₄:Tm and MgSO₄:Dy,Mn thermoluminescence (TL) phosphors have been prepared and their emission spectra were measured using a linear heater and optical multichannel analyzer. Emission bands at about 480, 580 and 660 nm of MgSO₄ doped with Dy were observed in three dimension (3D) glow curve. Emission bands about 360, 460, and 660 nm were observed in a 3D glow curve of MgSO₄ doped with Tm. The emission spectra of MgSO₄:Dy and MgSO₄:Tm are attributed to the characteristic emission wavelengths from transitions of Dy³⁺ and Tm³⁺ respectively. The results show that the structures of traps in matrix materials determine the activation energy distribution and dopant energy levels of rare earth ions are related with the emission spectrum wavelengths of sulfate phosphors. The intensities of the glow peaks in both bands at about 480 and 580 nm in MgSO₄ doped Dy and Mn were dramatically reduced in comparison with that of MgSO₄ doped Dy except above 300°C. It means that the trapping structures of MgSO₄ :Dy phosphor has greatly been altered by the co-dopant Mn but no change is observed in wavelengths of the emission spectra.     

Synthesis and luminescent properties of BaGd2O4:Dy3+, an novel scintillating phosphor

The BaGd_2?x O₄:xDy³⁺ (0 ≤ x ≤ 0.08) phosphors were synthesized at 1,300 °C in air by the solid-state reaction route. The as-synthesized phosphors were characterized by X-ray powder diffraction, photoluminescence excitation spectra, photoluminescence (PL) spectra, X-ray excited luminescence (XEL) spectra, and thermoluminescence (TL) spectra. It is found that the quenching concentration of Dy³⁺ ions in BaGd₂O₄ host is dependent on the selected excitation wavelength. The optimal PL intensity for the investigated BaGd_2?x O₄:xDy³⁺ phosphors is found to be x = 0.01, 0.02, and 0.04, upon excitation by 234, 277, and 350 nm ultraviolet light, respectively. The energy transfer among Dy³⁺ ions upon excitation by 350 nm is confirmed to be an electric dipole–dipole interaction mechanism based on the fitting of Huang’s rule. In addition, the intensive XEL from BaGd₂O₄:Dy³⁺ phosphor is observed by the naked eyes at room temperature, and TL properties of the investigated phosphors are analyzed and discussed. All the results imply that the investigated phosphors could be a promising scintillating phosphor.     

Dy含量对红色长余辉发光材料Sr3Al2Ｏ6:Eu2＋,Dy3＋性能的影响

采用溶胶凝胶法制备了Sr₃Al₂Ｏ₆:Eu^2＋,Dy^3＋红色长余辉发光材料,利用X射线衍射仪对材料的物相进行了分析,结果表明,1200℃下制备的样品的物相为Sr₃Al₂Ｏ₆,少量的Eu和Dy掺杂没有影响样品的相组成.采用荧光分光光度计、照度计测定了样品的发光特性.结果表明Sr₃Al₂Ｏ关键词： 红色长余辉 3Al₂Ｏ₆')" href="#">Sr₃Al₂Ｏ₆ 溶胶凝胶法     

Hydrothermal synthesis and luminescent properties of LnPO4:Tb,Bi (Ln=La,Gd) phosphors under UV/VUV excitation

Monoclinic LnPO₄:Tb,Bi (Ln=La,Gd) phosphors were prepared by hydrothermal reaction and their luminescent properties under ultraviolet (UV) and vacuum ultraviolet (VUV) excitation were investigated. LaPO₄:Tb,Bi phosphor and GdPO₄:Tb phosphor showed the strongest emission intensity under 254 and 147 nm excitation, respectively, because of the different energy transfer models. In UV region, Bi³⁺ absorbed most energy then transferred to Tb³⁺, but in VUV region it was the host which absorbed most energy and transferred to Tb³⁺.