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1.
采用水热法合成了一种非稀土上转换发光材料,由钠铝氟化物和BaF2组成。采用X射线衍射(XRD)、傅里叶红外光谱(FTIR)和扫描电镜(SEM)对其进行了表征,分析表明,钠铝氟化物主要以NaF和Na3AlF6两种晶态存在于BaF2晶体表面,形成化学复合,呈现包覆结构。荧光光谱测试表明,样品在583nm可见光和863nm近红外光室温激发下,均能产生304和324nm的宽波段紫外光发射。时间分辨光谱表明,发光均有一个上升和衰减过程,衰减大约自15ms开始,磷光寿命大于18.4ms。借助上转换发光能量转换过程对发光机理进行了研究,分析表明,发光源于量子限制效应的带间光吸收和界面缺陷的光吸收,发光机制属于量子限制效应-界面发光中心复合发光。  相似文献   

2.
TmP5O14晶体的上转换发光的研究   总被引:1,自引:0,他引:1       下载免费PDF全文
报道室温下TmP5O14晶体在脉冲DCM染料激光激发下产生的紫外和深紫色上转换发光现象.测量发现在300—500nm波长范围内主要有两组上转换荧光,一是较强的1D23H6,3F4的360和450nm的双光子荧光,另一是1I6→3F4的347nm的三光于荧光,发现了由 关键词:  相似文献   

3.
采用水热法制备了一系列不同掺杂浓度的NaGdF4:Re(Re=Tm3+,Er3+,Yb3+)上转换发光粉。通过X射线衍射(XRD)、电子扫描电镜(SEM)和上转换发射光谱对样品进行了表征。XRD研究结果表明:合成的样品均为六方结构NaGdF4。估算的平均晶粒尺寸为41~43 nm。在980 nm红外光激发下,Er3+和Yb3+共掺杂的NaGdF4发光粉发出分别来自于Er3+离子2H11/ 2,4S3/24I15/2跃迁的绿光和4F9/24I15/2跃迁的红光发射,Tm3+和Yb3+共掺杂的NaGdF4发光粉发出分别来自Tm3+离子的1G43H6跃迁的蓝光、1G43F43F2,33H6跃迁的红光和3H43H6跃迁的近红外光发射。Er3+,Tm3+和Yb3+共掺杂的NaGdF4发光粉的发光强度及红、绿、蓝光发射的相对强度受Yb3+离子掺杂浓度的影响。对样品中可能的上转换发光机制进行了讨论。计算的色坐标显示:可通过改变掺杂离子浓度对上转换发光的颜色进行调控。  相似文献   

4.
制备了一系列Na1-xKxErF4@NaLuF4的核壳纳米结构,核中K+掺杂摩尔分数变化范围为0%~8%。XRD分析结果揭示这些具有不同K掺杂浓度的纳米粒子均为β-相纳米结构。研究结果表明:随着K+浓度的增加,纳米结构中Er3+~650 nm处的红带发光强度呈现先增强后减弱的规律,当K+摩尔分数为4%时,Na0.96K0.04ErF4@NaLuF4纳米晶的发光强度达到最大,为未掺杂K+的NaErF4@NaLuF4纳米晶发光强度的3.7倍。其发光增强的原因在于K+的掺杂降低了Er3+微环境晶场宇称对称性,提高了Er3+离子4F9/24I5/2能级辐射跃迁几率,进而增强了Er3+的650 nm红带的上转换发光强度。  相似文献   

5.
钪基氟化物化学性质稳定、声子能量低、无辐射弛豫概率较低,是一种新型高效的基质材料,并且Sc3+半径较小,能与多种氨羧络合剂形成稳定的螯合物,因而具有更加奇特的物理和化学性质,近年来,成为许多科学家研究的热点。以聚乙烯二胺(PEI)作为表面活性剂,采用水热法在反应温度为200 ℃时成功制备了ScF3∶Yb3+/Er3+,NaScF4∶Yb3+/Er3+,(NH4)2NaScF6∶Yb3+/Er3+纳米上转换发光材料。通过X射线衍射仪(XRD)、透射电镜(TEM)、扫描电镜(SEM)和荧光光谱仪对所制备样品的晶相、形貌和发光特性进行了研究,结果显示:通过改变反应物NH4F和Ln3+的比例(NH4F/Ln3+=1∶1,2∶1,2.5∶1,3∶1,4∶1,6∶1,10∶1,20∶1,30∶1,40∶1,50∶1)实现了对样品产物、晶相、形貌的控制。当NH4F/Ln3+为2.5∶1时,生成了纯立方相的ScF3;在NH4F/Ln3+为4∶1时,生成了六角相的NaScF4;在NH4F/Ln3+为40∶1时,生成了一种纯立方相的新型基质材料(NH4)2NaScF6,样品结晶度高,形貌均一,有正方形片状和足球状多面体;在980 nm红外激光的激发下,不同NH4F/Ln3+比例生成的样品发光呈现桔黄→桔红→绿→黄绿等多种颜色的变化。实验表明仅改变NH4F一种原料的用量,就可以生成ScF3∶Yb3+/Er3+,NaScF4∶Yb3+/Er3+和(NH4)2NaScF6∶Yb3+/Er3+ 三种不同的产物,说明NH4F的用量对产物的生成有决定性的作用,对晶相的转换、颜色的调控亦有重要影响。  相似文献   

6.
将Yb~(3+)作为协助发光的敏化剂,Tb~(3+)和Tm~(3+)作为发光中心的激活剂分别加入到基质氟化钇钠中,通过水热合成法分别制成不同掺杂浓度的NaYF_4:Yb~(3+)/Tb~(3+)和NaYF_4:Yb~(3+)/Tm~(3+)双掺杂氟化物纳米发光材料,并通过扫描电子显微镜、X射线衍射以及荧光光谱等手段分别对NaYF_4:Yb~(3+)/Tb~(3+)和NaYF_4:Yb~(3+)/Tm~(3+)双掺杂氟化物材料纳米颗粒的形貌及其发光特性进行了研究.实验结果表明:系列样品的X射线衍射图谱衍射峰与标准卡片吻合得很好,实验浓度范围内Yb~(3+)/Tb~(3+)和Yb~(3+)/Tm~(3+)共掺没有改变NaYF_4的晶体结构.实验得到了该材料在980 nm激光激发下的上转换发光光谱并分析了该材料的上转换发光机理,NaYF_4:Yb~(3+)/Tb~(3+)在980 nm激光激发的情况下出现的蓝光,绿光以及红光,分别对应于~5D_4→~7F_6、~5D_4→~7F_5、~5D_4→~7F_1的辐射跃迁;NaYF_4:Yb~(3+)/Tm~(3+)在980 nm光源激发下出现强的480 nm的蓝光,对应的是~1G_4→~3H_6的电子跃迁能级带,在660 nm强的红光发射谱带,对应的是~1G_4→~3F_4能级跃迁辐射光.  相似文献   

7.
在980 nm LED激光器激发下,研究了Yb3+-Er3+共掺杂的Y2O3,Y2O2S和NaYS2粉末材料的上转换发射特性。比较了Y2O3∶0.20 Yb3+,0.03Er3+和Y2O2S∶0.20 Yb3+,0.03Er3+以及NaYS2:0.20 Yb3+,0.03Er3+粉末样品的上转换发光光谱,探讨了Er3+上转换发射对基质的依赖性,分析了S2--Yb3+和S2--Er3+电荷转移态对Yb3+-Er3+间能量传递和能级间跃迁几率的影响,借助于能级图解释了在不同基质中Yb3+-Er3+间的能量传递和Er3+的上转换发光机制。  相似文献   

8.
稀土掺杂材料的上转换发光   总被引:2,自引:0,他引:2  
稀土掺杂材料的上转换发光是实现光波频率转换的重要途径,也是稀土掺杂发光材料研究的重要内容。本文从介绍与上转换相关的基本概念出发,阐述了稀土离子上转换发光的发展历史;对稀土离子掺杂材料的能量传递、激发态吸收、合作敏化、合作发光、双光子吸收激发及光子吸收雪崩等上转换发光机制进行了概述,并对各机制进行了比较;对不同稀土离子掺杂体系中上转换发光的机制进行了总结;对以往研究的稀土掺杂上转换发光材料的基质,包括粉体材料、晶体材料、非晶材料进行了概括;最后对影响稀土离子上转换发光效率的因素进行了分析,提出了在上转换发光材料的设计中应重点考虑基质对泵浦光及上转换发射光的吸收、基质材料的声子能量、稀土离子的掺杂方案及泵浦途径等因素。  相似文献   

9.
基质发光材料Na5Eu(MoO4)4和NaEu(MoO4)2的制备和发光   总被引:1,自引:0,他引:1  
郭常新  李碧琳 《发光学报》1991,12(2):118-126
本文研究了化学计量的基质发光材料Na5Eu(MoO4)4和NaEu(MoO4)2.它们都属于四方晶系,空间群为I41/α .NaEu(Mo04)2属于白钨矿(scheelite)结构,一个晶胞中有2个分子式NaEu(MoO4)2(z=2);而Na5Eu(Mo4O)4属于类自钨矿(scheelite-like)结构,一个晶胞中有4个分子式Na5Eu(MoO4)4(z=4).X射线衍射确定的晶胞常数,对Na5Eu(MoO4)4,α=1.1439nm和c=1.1486nm(密度d计算=4.01g/cm3,z=4);对NaEu(MoO4)2,α=0.5236nm和c=1.1439nm(密度d计算=5.24g/cm3,z=2).由差热法和X射线衍射法确定了Na2MoO4-Eu2(MoO4)3的相图.Na5Eu(MoO4)4分解为NaEu(MoO4)2的温度是700℃.本文确定了制备纯 Na5Eu(MoO4)和NaEu(MoO4)2的方法,并研究了上述两种材料的激发光谱和发光光谱.确定了用X射线粉末衍射谱和发光光谱鉴别Na5Eu(MoO4)4和NaEu(MoO4)2的方法.在365nm紫外光激发下,Na5Eu(MoO4)4的发光比Na5Eu(WO4)4的强得多,在室温下,Na5Eu(MoO4)4,NaEu(MoO4)2和Na5Eu(WO4)4的相对发光积分亮度比为3.8:3.2:1.0.  相似文献   

10.
HoYb:YVO4的上转换发光研究   总被引:2,自引:0,他引:2       下载免费PDF全文
研究了960nm激光激发下HoYb双掺钒酸钇晶体HoYb:YVO4的直接上转换增敏发光,发现了Ho3+离子的上转换发光现象,HoYb:YVO4晶体的上转换发光是5F5→5I8最强,而5S2→5I8相对小了一个数量级,这是由于YVO4晶体既有很强的振子强度又有很大的多声子无辐射弛豫造成的. 关键词: 上转换发光 直接增敏(敏化) 钒酸钇YVO4晶体 Ho3+离子  相似文献   

11.
谢晔  王涛  王海波 《发光学报》2010,31(6):821-825
采用化学共沉淀法对Y(PV)O4∶Eu3+荧光粉进行表面包膜处理,获得了表面均匀包覆Y(OH)3膜层的Y(PV)O4∶Eu3+荧光粉。用SEM、XRD等手段对其表面形貌、晶格结构性能进行了表征。结果表明:在Y(PV)O4∶Eu3+粉体表面均匀包覆Y(OH)3膜层后,Y(PV)O4∶Eu3+的晶格结构、发光性能没有改变,亮度较未包覆的荧光粉有较大提高,且没有发生色坐标偏移现象。  相似文献   

12.
Intense green‐emitting Li(Gd,Y)F4:Yb,Er/LiGdF4 core/shell (C/S) upconversion nanophosphors (UCNPs) with a tetragonal bipyramidal morphology are synthesized. The morphology and UC luminescence of the Li(Gd,Y)F4:Yb,Er UCNPs are significantly affected by the Li precursors, and bright UC green‐emitting Li(Gd,Y)F4:Yb,Er UCNPs with a tetragonal bipyramidal shape, i.e., UC tetragonal bipyramids (UCTBs), are synthesized using LiOH·H2O as a Li precursor. A LiGdF4 shell is grown on the Li(Gd,Y)F4:Yb,Er UCTBs, and the C/S UCNPs exhibit 4.7 times higher luminescence intensity than core UCTBs. The C/S UCNPs show a high absolute UC quantum yield of 4.6% under excitation with 980 nm near infrared (NIR) light, and the UC luminescence from the C/S UCNPs is stable under continuous irradiation with the 980 nm NIR laser for 1 h. The hydrophobic surfaces of the as‐synthesized C/S UCNPs are modified to hydrophilic surfaces by using poly(acrylic acid) (PAA) for bioimaging applications. They are applied to human cervical adenocarcinoma (HeLa) cell imaging and SK‐MEL‐2 melanoma cell imaging and in vivo imaging, including subcutaneous and intramuscular imaging, and UC luminescence images with high signal‐to‐noise ratio are obtained. Furthermore, sentinel‐lymph‐node imaging is successfully conducted with the PAA‐capped Li(Gd,Y)F4:Yb,Er/LiGdF4 C/S UCNPs under illumination with NIR light.  相似文献   

13.
Copper-doped Na21(SO4)7F6Cl phosphor was synthesized via the conventional wet chemical method. The synthesis was carried using CuCl2 and Cu (NO3)2·3H2O as dopants in two different steps successively. The formation and phase purity of the compound were revealed by the X-ray diffraction pattern. Functional groups of the prepared phosphor were observed in the FT–IR spectrum. The emission along with excitation spectra were followed to explore the luminescence attributes. Photoluminescence (PL) emission spectrum of the material synthesized using CuCl2 as the dopant was observed at 358?nm due to 3dl0?3d94s transitions when excited around 247?nm for various copper concentrations. Efficient blue emissions were obtained at peaks 423 and 469?nm for materials synthesized using Cu (NO3)2·3H2O as the dopant, when monitored at 357?nm excitation. The Commission Internationale de I’Eclairage chromaticity coordinates for different copper concentrations were calculated for the emission around 423?nm. TL glow curves of Na21(SO4)7F6Cl:Cu phosphor for different dopant concentrations, irradiated with 100?Gy gamma dose, were studied and hence the trap parameters, namely order of kinetics (b), activation energy (E) and frequency factor (s) associated with the most intensive glow peak of Na21(SO4)7F6Cl:Cu phosphor were determined by using Chen’s Peak shape method. The results indicate that Na21(SO4)7F6Cl:Cu+ is a potential novel blue-emitting lamp phosphor and may be quite suitable for use in dosimetry of ionizing radiations.  相似文献   

14.
Yb3+:KGd(WO4)2材料的频率上转换发光   总被引:3,自引:0,他引:3  
采用固相合成法 ,在 10 0 0℃烧结合成了一系列掺有Yb3 摩尔分数分别为x =0 0 3,0 0 8,0 10 ,0 12 ,0 15 ,0 18,0 2 0 ,0 2 5 ,0 2 8的KYbxGd( 1 -x) (WO4 ) 2 粉末样品。采用 980nm波长的LD泵浦源和RF 5 4 0荧光光谱仪 ,对这一系列掺有不同Yb3 摩尔分数的KYbxGd( 1 -x) (WO4 ) 2 粉末样品进行了荧光光谱的测定研究。结果表明 ,在 10 2 0nm处得到一个较弱的荧光峰 ,而在 4 76nm处得到很强的蓝色发光谱带。同时测定了蓝色发光强度与样品掺杂Yb3 摩尔分数的关系 ,随着Yb3 掺杂摩尔分数的增加 ,蓝色发光强度也随着迅速地增强 ,当Yb摩尔分数为 2 5 %时 ,荧光强度达到最大 ,然后 ,随着Yb掺杂摩尔分数的增加 ,蓝色发光强度也随着迅速地衰弱。当Yb掺杂摩尔分数为 8%~ 10 % ,10 2 0nm处的荧光强度达到最大。  相似文献   

15.
In the present paper Na3SO4Cl:Ce, Na3SO4Cl:Dy, Na3SO4Cl:Mn, of Na3SO4Cl:Ce, Dy and Na3SO4Cl:Ce, Mn phosphor were synthesized by the wet chemical method. Thermoluminescence (TL) characteristics of Na3SO4Cl:Ce, Na3SO4Cl:Dy, Na3SO4Cl:Mn, Na3SO4Cl:Ce, Dy and Na3SO4Cl:Ce, Mn phosphors were studied for 5 Gy γ-ray dose. In TL glow curve, two peaks have been observed at 129°C and 224°C for different concentrations of Ce and Dy, whereas Mn peaks at 212°C. The same host is also tried for Ce, Dy (peaks at 126, 219) and Ce, Mn (248°C). A significant single peak is observed in the case of Na3SO4Cl:Mn and Na3SO4Cl:Ce, Mn. This may be due to the effect of activators. It is found that intensity tends to be increase with increased concentrations of the activators. The TL glow curves of the phosphors have been recorded and irradiated at a rate of 0.39 kGy h?1 for 5 Gy γ-rays dose. It is also found that all the phosphors are less sensitive as compared with Thermoluminescence dosimetry-CaSO4: Dy for the same γ-rays dose. The paper discuses the preliminary TL characteristics and effect of γ-rays on Na3SO4Cl:Ce, Na3SO4Cl:Dy, Na3SO4Cl:Mn, Na3SO4Cl:Ce, Dy and Na3SO4Cl:Ce, Mn phosphors.  相似文献   

16.
(Sr,Ca)AlSiN3:Eu2+红色荧光粉在热性能和长期使用性能等方面还有一定差距,导致制成的白光LED在长期工作状态下发生光衰和色标漂移,影响了白光LED的品质。为解决这一问题,将微量碱土金属离子和稀土金属离子掺入(Sr,Ca)AlSiN3:Eu2+中,研究其对(Sr,Ca)AlSiN3:Eu2+红色荧光粉热性能和长期使用性能的影响。实验结果表明:Li+-Dy3+、Li+-Ho3+等碱土金属-稀土金属离子对(Sr,Ca)AlSiN3:Eu2+红色荧光粉的光衰性能有较明显的提升,同时也显著减小了制灯后长时点亮的色漂移。  相似文献   

17.
研究了提拉法生长的掺Er^3+的Sr3Y2(BO3)4晶体的吸收光谱和荧光光谱。应用J—O理论分析并计算了光谱参数,得到唯象参数Ω2、Ω4和Ω6分别为11.90×10^-20cm^2、3.44×10^-20cm^2和1.92×10^-20cm^2。在Er^3+:Sr3Y2(BO3)4晶体中,Er^3+在1533nm波长的发射截面为1.00×10^-20cm^2,^4I13/2→^I15/2能级跃迁的荧光寿命和辐射寿命分别为0.58ms和4.10ms,良好的光谱性能表明Er^3+:Sr3Y2(BO3)4晶体可能成为潜在的1.55μm波段的一种激光材料。  相似文献   

18.
共沉淀法制备Y(P,V)O4:Tm3+荧光粉及其光致发光   总被引:1,自引:2,他引:1  
采用氨水、双氧水和磷酸氢二铵溶液作沉淀剂,通过共沉淀法制备出Y(P,V)O4:Tm^3 荧光粉,利用XRD、SEM、紫外以及真空紫外激发下的发射光谱对其进行研究。结果表明:共沉淀法制备的Y(P,V)O4:Tm^3 荧光粉的颗粒形貌好,在147nm真空紫外光和254nm紫外光激发下,荧光粉发射主峰位于476nm,色坐标范围为:0.167≤x≤0.200;0.146≤y≤0.183。从这些结果来看,Y(P,V)O4:Tm^3 体系还不能满足实际应用的要求,仍需进一步的深入研究以改善其性能。  相似文献   

19.
Spectroscopic characterization of Yb3+/Er3+ codoped TeO2–R2O–ZnO–Ln2O3 glasses as a function of network modifiers (R=Li, Na and K) has been investigated. The Judd–Ofelt parameters (Ωt), quantum efficiency in near infrared (1.55 μm) and visible up-conversion (546 and 660 nm) and quality factor spectroscopy (χ) were calculated. Three up-conversion emission bands centered at 525, 546 and 660 nm were observed as maxima for glasses containing potassium. The measured lifetime of 4I13/2, 4F9/2 and 4S3/2 from Er3+ and 4F5/2 from Yb3+ levels increased when potassium (K) replaced lithium (Li) and Na. The maximum emission cross-section (ECS) for 4I13/24I15/2 transition of Er3+ was calculated to be 1.02×10?20 cm2 for TeO2–Li2O–ZnO–Ln2O3 glasses. The energy transfer efficiency (ET) from Yb3+ to Er3+, (4F5/2)+(4I15/2)→(4F7/2)+(4I13/2), was calculated using the measured lifetimes of Yb3+ with and without the presence of acceptor (Er3+). The maximum calculated ET was 58% for 0.25 mol% of Er3+ and 3 mol% of Yb3+ for TeO2–K2O–ZnO–Ln2O3 glass composition.  相似文献   

20.
We have investigated the optical and scintillating properties of Lu co-doped Ce:LiYF4 single crystals with various Lu content. In the transmittance and absorption spectra, the absorption peaks at 243 nm get systematically red shifted in contrast to the peaks at 197 and 200 nm which get blue shifted with the increase in Lu content. At the same time, emission peaks at 306 nm and 200 nm under 295 nm excitation also get red shifted. The decay time of Ce:Li(Y,Lu)F4 crystals under 295 nm excitation is found to be faster than that of Ce:LiYF4 and Ce:LiLuF4 crystals. The alpha-peak positions in the pulse-height spectra and decay times of crystals under alpha-ray irradiation are found to vary with the Lu content.  相似文献   

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