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1.
研究了以尿素为沉淀剂,通过改变加热方式、溶液pH、Eu~(3+)掺杂量及煅烧温度等条件,采用微波辅助液相法制备Y_2O_3:Eu~(3+)红色荧光粉,并对所得荧光粉进行检测分析。结果表明:试验所制备的荧光粉为规整的球形,涂敷性好,可以被近紫外激发光有效激发,发射主峰位于614nm处,归属于Eu~(3+)的~5 D_0→~7 F_2跃迁;该红色荧光粉可应用在白光LED。  相似文献   

2.
《中国钨业》2017,(3):65-70
采用高温固相法合成了NaGd(WMo)O_(8-x/2)F_x:Eu~(3+)(x=0、0.1、0.2、0.3、0.4、0.5)系列红色荧光粉。分别采用X射线衍射、荧光光谱测试手段对所得粉末的晶型及其发光性能进行了表征分析。结果表明,该系列红色荧光粉均为白钨矿四方晶系结构,空间点群结构为I41/a(88),可被近紫外光395 nm有效激发,其最强发射峰位于616 nm处,属于Eu~(3+)的~5D_0→~7F_2电偶极跃迁。F-离子掺杂量为0.2 mol时发光强度最强,与未掺杂F-相比其发光强度提高了41%,其色坐标为(0.653,0.336)。由此可见,NaGd(WMo)O_(7.9)F_(0.2):Eu~(3+)是一种具有潜在应用价值的白光LED红色荧光粉。  相似文献   

3.
以MgMoO_4为基质,Eu~(3+)为激活剂,NH_4Cl为助熔剂,采用高温固相法合成白光LED用MgMoO_4:Eu~(3+)红色荧光粉。通过差示扫描量热与热重分析(DSC/TG)研究合成荧光粉的最佳温度,利用X射线衍射仪(XRD)、扫描电镜(SEM)和傅里叶红外光谱仪(FT-IR)研究荧光粉的结构,并用荧光光谱仪对荧光粉的发光效果进行检测。结果表明:用NH_4Cl作为助熔剂,合成MgMoO_4:Eu~(3+)荧光粉的最佳温度为900℃。添加NH_4Cl后,MgMoO_4:Eu~(3+)荧光粉的结构得到优化,颗粒呈椭球形,粒径约为0.5~1μm。395 nm和465 nm波长激发的发射光谱由一系列尖峰组成,分别位于592 nm(~5D_0→~7F_1),615 nm(~5D_0→~7F_2)和699 nm(~5D_0→~7F_4)处,其中615 nm处的发射峰强度最大,属于Eu~(3+)的超灵敏电偶极跃迁。添加NH_4Cl可明显提高MgMoO_4:Eu~(3+)荧光粉的激发与发射峰的强度,最佳添加量(n(NH_4Cl)/n(MgO))为1%,此时发射光谱的强度是未添加NH_4Cl时的7倍左右,395 nm激发的发射光谱对应的最佳Eu~(3+)浓度为0.1,465 nm激发的发射光谱对应的最佳Eu~(3+)浓度为0.15。  相似文献   

4.
采用高温固相法制备了K_2Gd_(1-x-y)(PO_4)(WO_4):x Sm~(3+),y Eu~(3+)新型红色荧光材料,通过利用X射线衍射谱(XRD)、荧光光谱对其结构及发光性能进行了研究。结果表明,稀土离子S~(3+)的掺入没有改变荧光粉的晶相;样品的激发光谱在394 nm有很强的激发峰,与近紫外LED芯片匹配,且Eu~(3+)的~5D_0→~7F_2电偶极跃迁表现出616 nm有较好的红光发射,Eu~(3+)的最佳掺杂量(摩尔分数)为y=0.3;Sm~(3+)进入晶格后,激发峰明显增强和变宽,表明Sm~(3+)对Eu~(3+)的发光起到敏化作用;K_2Gd_(0.68)(PO_4)(WO_4)∶0.3Eu~(3+),0.02Sm~(3+)样品在150℃时发光强度仍为初始温度的78%,具有良好的热稳定性且色纯度高,是一种潜在的白光LED用荧光粉。  相似文献   

5.
采用高温固相反应法制备了一系列Li+掺杂的Ca(W,Mo)O_4∶Eu~(3+)荧光粉。通过X射线衍射仪、扫描电子显微镜及荧光光谱仪对样品的结构、形貌及荧光性能进行了表征。XRD及SEM结果表明,Li~+掺杂没有改变样品原有的四方晶系体心结构,Li+能够以替代和间隙掺杂的方式进入主晶格,适当的Li+掺杂可以改善样品的团聚现象。样品的激发光谱涵盖200~550nm的宽带激发,在395nm激发下,能发射出位于616nm处的窄带红光,归因于Eu~(3+)的~5D_0→~7F_2跃迁,适量Li~+的掺杂明显提升了样品的发光强度。与其他碱金属离子(Na~+、K~+)掺杂相比,Li~+由于半径最小、电负性最强,使得发光强度增强最多。  相似文献   

6.
采用高温固相法在1200℃、保温3 h的条件下制备了(Sc,Y)(V_(1-x)B_x)O_(4-x):Eu~(3+)(0≤x≤0.5)系列样品,通过荧光光谱仪、X射线衍射仪(XRD)、扫描电子显微镜(SEM)对粉体的荧光性能、结构及形貌进行测试和表征。结果表明,在365 nm紫外光激发下,荧光粉主发射波长位于620 nm,对应于Eu~(3+)的~5D_0→~7F_2跃迁,当x=0.1时,相对发光强度是Sc_(0.73)Y_(0.2)VO_4:Eu_(0.07)~(3+)的1.6倍;在620 nm监控下,存在一个峰值位于337 nm的极强宽带吸收带和396 nm处的弱激发带。与(Sc,Y)VO_4:Eu~(3+)相比,硼的掺杂没有改变样品的四方晶系体心结构,且形貌未发生明显改变,粒度分布均匀、无明显团聚。在397 nm激发下,荧光粉的内量子效率提升了2倍,当温度升高至200℃,其相对发光强度仍保持在92%,显现出高的内量子效率和低的热淬灭效应,适合近紫外激发白光发光二极管(LED)用红色荧光粉。  相似文献   

7.
Fluorescence spectra of Sm~(2+)and Eu~(2+)→Sm~(2+)energy transfer were studied in SrB_4O_7.There appearsonly fluorescence from ~5D_0 transition of Sm~2+ at 77 K.The vibronic lines associated with ~5D_0→~7F_0 transitionwere observed.The thermal population to upper states of ~5D_1 and 4f~5d levels from ~5D_0 gives rise to ~5D_1→~7F_J and 5d→4f radiative transitions of Sin~(2+)at higher temperature.  相似文献   

8.
In this study,α-TeO_2:Ho~(3+)/Yb~(3+),α-TeO_2:Eu~(3+) and α-TeO_2:Ho~(3+)/Yb~(3+)/Eu~(3+) nanoparticles were prepared via a simple hydrothermal process.The up- and down-conversion properties of the as-prepared nanoparticles were tested at room temperature under a near-infrared photo source(980 nm) and UV-vis photo source,respectively.The results indicated that α-TeO_2 NPs were a kind of outstanding host material for both up- and down-conversion luminescence.The α-TeO_2:Ho~(3+)/Yb~(3+) nanoparticles showed sharp up-conversion emission at 545 and 660 nm under 980 nm excitation,ascribed to the ~5S_2→~5I_8 and ~5F_5→~5I_8(Ho~(3+)) transitions,and weaker down-conversion emission at 545 nm under 455 nm excitation,ascribed to the ~5S_2→~5I_8(Ro~(3+)) transitions.The α-TeO_2:Eu~(3+)nanoparticles showed strong down-conversion emission at 592 and 615 nm under 395 nm excitation,attributed to the ~5D_0→~7F_1 and~5D_0→~7F_2(Eu~(3+)) transitions.Possessing the advantages of these two luminescent materials,the as-prepared tri-doped samples ofα-TeO_2:0.5Ho~(3+)/10Yb~(3+)/3Eu~(3+)(mol.%) nanoparticles could successfully emit visible light via both up- and down-conversion modes.  相似文献   

9.
以DEG为溶剂,分别配置一定比例的GdCl_3, TbCl_3作为前驱液,利用多元醇法合成可用于生物探针的Gd_2O_3:Tb~(3+)纳米晶;将一定量的APTES和TEOS加入制备好的溶液中,使得纳米晶Gd_2O_3:Tb~(3+)的表面包裹聚硅氧烷层。本实验通过马尔文粒度仪、 X射线衍射仪(XRD)、场发射扫描电镜(SEM)、透射电镜(TEM)、荧光分光光度计等检测方法研究不同煅烧温度和不同Tb~(3+)掺杂浓度对纳米晶Gd_2O_3的粒径、物相结构、和发光性能的影响。将真空干燥过的纳米晶Gd_2O_3:Tb~(3+)置于马弗炉中分别以600, 800, 1000℃进行煅烧,得到的样品经XRD表征后发现:当煅烧温度为800℃时,得到立方相结构的纳米Gd_2O_3:Tb~(3+)。通过研究不同Tb~(3+)离子掺杂浓度下纳米晶Gd_2O_3:Tb~(3+)的荧光强度表明:当Tb~(3+)离子浓度为5.0%时,纳米晶Gd_2O_3:Tb~(3+)的发射强度最强,尤其是在主发射峰545 nm附近Tb~(3+)的~5D_4→~7F_5能级跃迁峰,其峰值强度比掺杂浓度为2.5%时提高了39%; Tb~(3+)掺杂浓度升高至7.5%时,样品发生了浓度猝灭导致光谱强度下降。  相似文献   

10.
《稀土》2021,(1)
以Gd_2O_3、Eu_2O_3和NH_4HSO_4为原料,采用微波辐射法合成了Gd_2O_2SO_4∶Eu~(3+)发光材料。并用X射线衍射仪、扫描电镜、荧光光谱仪对所得发光材料的物相、形貌和发光性能进行了表征。结果表明,微波辐射30 min可以合成纯相Gd_2O_2SO_4∶Eu~(3+)发光材料,晶体结构为正交晶系,与Gd_2O_2SO_4结构相同;其形貌不规则,存在团聚现象;Gd_2O_2SO_4∶Eu~(3+)发光材料呈红光发射,发射光谱由一系列铕离子的~5D_0→~7F_j(j=0,1,2,3,4)能级跃迁的尖峰组成,激发光谱主要由处于200 nm~350 nm的宽激发带和位于397 nm和466 nm的窄激发带组成。  相似文献   

11.
采用高温固相法制备了一系列的NaY_(0.78-x)(MoO_4)_2∶0.2Yb~(3+),0.02Ho~(3+),xZn~(2+)(x=0,0.05,0.1,0.15,0.2,0.25)荧光粉。通过X射线衍射仪、扫描电镜以及荧光光谱仪分别对样品的结构、形貌和荧光性能进行了表征。结果表明Zn~(2+)的掺杂可以通过替换Y~(3+)格位和占据晶格间隙的方式进入基质晶格。在980nm激光激发下,样品呈现出了强烈的绿光(551nm)和相对微弱的红光发射(668nm),分别归因于Ho~(3+)的~5F_4,~5S_2→~5I_8和~5F_5→~5I_8跃迁。Zn~(2+)的掺杂可以使上转换发光强度显著增强,其原因是Zn~(2+)掺杂产生了O~(2-)空位而且可以裁剪Ho~(2+)周围的局域晶体场对称性。基于泵浦依赖的研究,对能级图和可能的上转换发光机理进行了详细的讨论。  相似文献   

12.
采用共沉淀法制备了Ca_(0.93-x)(Mo_(0.9)W_(0.1))O_4∶Eu_(0.07)~(3+),Bi_x~(3+)(0≤x≤0.05)系列样品,通过XRD、SEM及荧光光谱仪对粉体的晶体结构、形貌及荧光性能进行测试和表征。结果表明,Bi~(3+)、Eu~(3+)及WO_4~(2-)的掺杂没有改变CaMoO_4原有的四方晶系体心结构,且样品粒径分布较均匀,无明显团聚现象。随着Bi~(3+)的掺杂,Ca_(0.93-x)(Mo_(0.9)W_(0.1))O_4∶Eu_(0.07)~(3+),Bi_x~(3+)样品的激发光谱带边会发生红移,且激发强度呈现先增强后减弱的趋势,其发射光谱也具有相应的规律,Bi~(3+)的最佳掺杂浓度为x=0.02 mol,在395 nm激发下,样品的发光强度提升至134%;较之商用红色荧光粉Y_2O_2S∶Eu~(3+),Ca_(0.91)(Mo_(0.9)W_(0.1))O_4∶Eu_(0.07)~(3+),Bi_(0.02)~(3+)样品显现出更好的色纯度和发光强度,适合于近紫外LED用红色荧光粉。  相似文献   

13.
Ca_3–xAl_2O_6:x Eu~(3+)(0.02≤x≤0.10) and Ca_(2.92)Al_2O_6:0.04Eu~(3+),0.04M~+(M~+=Li~+, Na~+, and K~+) phosphors were prepared by sol-gel method and their photoluminescence properties were investigated. The crystal structure of the annealed Ca_3–xAl_2O_6:x Eu~(3+) and Ca_(2.92)Al_2O_6:0.04Eu~(3+),0.04M~+ phosphors was analyzed with X-ray diffraction(XRD). The size and morphological characteristics of the annealed phosphors were investigated with a field emission scanning electron microscope(FE-SEM). The photoluminescence properties were evaluated with a spectrofluorometer. The phosphors were effectively excited by the light of 396 nm and showed intense red emission at 616 nm, which originated from the 5D_0→7F_2 transition of Eu~(3+). Among the prepared phosphors, the Ca_(2.96)Al_2O_6:0.04Eu~(3+) phosphor showed the strongest emission intensity and the highest color purity. The addition of alkaline metal ions(Li~+, Na~+, and K~+) to Ca_(2.96)Al_2O_6:0.04Eu~(3+) phosphor degraded the emission intensity and color purity.  相似文献   

14.
采用水热法制备具有单一相六方晶系的LaF_3:Eu~(3+)纳米荧光粉.通过X射线粉末衍射(XRD)、扫描电镜(SEM)、透射电镜(TEM)、光致发光光谱(PL)和荧光衰减曲线对LaF_3:Eu~(3+)纳米荧光粉进行表征. LaF_3:Eu~(3+)荧光粉的激发光谱主要由250 nm处的宽带(O2-→Eu3+的电荷转移跃迁)和一些尖峰(Eu3+f-f跃迁)构成,其中位于近紫外区396 nm处有一较强的激发峰.通过发射光谱探测Eu3+在LaF3晶体中的局部晶场环境.在298 K下激发光谱和发射光谱可知,在六方晶系的LaF3纳米晶体中的Eu3+晶格位置从D4h降至到C2v,这是由于晶格变化所造成的.在396 nm激发下,观测到较优掺杂浓度为10%的LaF_3:Eu~(3+)荧光粉在591 nm(5D0→7F1跃迁)处有强烈的红色发射峰.其发光性能表明,LaF_3:Eu~(3+)红色荧光粉在近紫外发光二极管领域具有潜在的应用价值.  相似文献   

15.
Tb~(3+)/Eu~(3+) co-doped transparent glass ceramics containing CaF_2 nanocrystals were successfully synthesized by high temperature melt-quenching method and subsequent heating. The structure and morphology of the samples were investigated by X-ray diffraction(XRD), transmittance electron microscopy(TEM), high resolution TEM(HRTEM) and selected area electron diffraction(SAED). The photoluminescence properties and energy transfer process from Tb~(3+) to Eu~(3+) of CaF_2:Tb~(3+),Eu~(3+) phosphors were also investigated through excitation spectra and decay curves. In addition, the emission spectra of the glass ceramics in a wide temperature range from 21 to 320 K were recorded under the excitation of 485 nm. It was found that the fluorescence intensity ratios of Tb~(3+) at 545 nm(~5D_4→~7F_5) to Eu~(3+) at 615 nm(~5D_0→~7F_2) was highly temperature-dependent with an approximate linear relationship, and the temperature sensitivity was about 0.4%/K. It is expected that the investigated Tb~(3+)/Eu~(3+) co-doped CaF_2 glass ceramics may have prospective application in optical thermometry.  相似文献   

16.
《稀土》2017,(2)
本文采用溶胶-凝胶法制备了Sr_(2-x-y)Ca_yAl_2SiO_7:xEu~(2+)(y=0,0.1,0.2,0.3,x=0.04)荧光粉,系统地研究了Ca~(2+)对Sr_2Al_2SiO_7:Eu~(2+)长余辉材料的微观结构和发光性能的影响,以及产生这些影响的机理。通过XRD与SEM分析,发现荧光粉为Sr_2Al_2SiO_7结构且为四方晶系,粒度在70 nm左右。对荧光粉的激发和发射光谱进行了测试,结果表明掺杂Ca~(2+)会使发射峰位置微弱蓝移并当浓度超过0.2%(摩尔分数,下同)后,出现浓度猝灭现象。采用三指数函数模型对余辉衰减曲线进行拟合,发现掺杂Ca~(2+)浓度为0.2%时光子的最大寿命为109 s大于未掺杂Ca~(2+)时的106 s。通过热释光谱测量,估算了其陷阱的深度和密度。分析表明,掺杂Ca~(2+)浓度为0.2%时荧光粉具有较佳的陷阱深度(0.77 eV)与陷阱密度(3.86×10~4(cm~3)~(-1)),表现出优良的余辉性能。  相似文献   

17.
《稀土》2016,(3)
采用高温固相反应合成了SrAl_2O_(4-y)N_y∶Eu~(2+),Dy~(3+)系列长余辉荧光粉,并研究了SrAl_2O_(3.75)N_(0.25)∶Eu~(2+),Dy~(3+)体系的晶体结构、光谱特性、余辉衰减曲线及热释发光曲线。X射线衍射分析结果表明,SrAl_2O_(3.75)N_(0.25)∶Eu~(2+)荧光材料属六方晶系,P6322空间群,晶胞参数a=b=5.14,c=8.462,γ=120°。荧光光谱测试结果表明,SrAl_2O_(3.75)N_(0.25)∶Eu~(2+)的激发光谱和发射光谱均为宽带谱,激发光谱位于283 nm~450 nm,发射光谱的峰值位于487 nm,属于Eu~(2+)的4f65d1→4f7跃迁发射。Eu~(2+)的掺杂量并不改变SrAl_2O_(3.75)N_(0.25)∶Eu~(2+)发射光谱的形状和峰值位置,但对相对发光强度有较大影响,Eu~(2+)的摩尔浓度为2%时相对发光强度最高。余辉衰减曲线表明,Sr_(0.97)Al_2O_(3.75)N_(0.25)∶Eu_(0.02),Dy_(0.01)的余辉衰减符合指数衰减规律,由初始的快衰减和之后的慢衰减两个过程组成。通过热释发光曲线对荧光材料中的陷阱能级进行计算,得出Sr_(0.97)Al_2O_(3.75)N_(0.25)∶Eu_(0.02),Dy_(0.01)的能级陷阱为0.42 V,掺Dy~(3+)有利于提高该荧光材料的初始发光亮度和余辉时间。  相似文献   

18.
研究采用高温固相法合成Eu~(3+),WO_4~(2-)共掺杂Na_2CaSiO_4系列红色荧光粉。通过X射线粉末衍射和荧光分析,研究荧光粉的结构和发光性能。考察了Eu~(3+),WO_4~(2-)掺杂量对荧光粉发光性能的影响。结果表明,掺杂了Eu~(3+),WO_4~(2-)后Na_2CaSiO_4仍为纯相,属立方晶系结构,但掺杂后晶胞参数发生变化,说明Eu~(3+),WO_4~(2-)已经进入晶格中。荧光粉发光强度随Eu~(3+),WO_4~(2-)掺杂含量的增加而增大。Eu~(3+)在晶体中的含量为20%时(以Na_2CaSiO_4物质的量为基准),荧光粉Na_2CaSiO_4∶Eu~(3+)的发光强度达到最大值。当WO_4~(2-)在晶体中的含量为0.07%时,此时,发射光的强度是掺杂前的2.74倍,色坐标为(0.66,0.34),更接近标准色坐标(0.67,0.33)。  相似文献   

19.
《稀土》2016,(2)
利用静电纺丝和高温煅烧相结合的方法制备了一维Eu~(3+)掺杂In_2O_3无机纳米纤维,并对其发光性能和发光机理进行研究。借助SEM、TG、XRD和EDX对样品的形貌、热分解、晶相和成分进行分析,利用荧光分光光度计测试了样品在室温下的光致发光性能。结果显示,静电纺Eu~(3+)掺杂前驱体纤维成型良好,经700℃煅烧5 h制备的In_2O_3∶Eu~(3+)纳米纤维仍保持纤维状形貌,但纤维直径与前驱体纤维相比明显减小;样品XRD衍射峰均与立方铁锰矿型In2O3的衍射峰一致,没有出现Eu_2O_3的衍射峰,样品EDX能谱分析表明煅烧后样品中含有In、O、Eu元素,且Eu含量与实际掺杂浓度接近。样品的室温发射光谱显示,经290 nm光激发后,在597 nm、612 nm和629 nm处出现Eu3+的发射峰,其中612 nm处的发射峰强度最大。  相似文献   

20.
The BaGd_(2-2 x)Eu_(2 x)O_4(BG, x = 0.01-0.09) phosphors were successfully synthesized via the sol-gel method,and BaY_(2-2 y)Eu_(2 y)O_4(BY, y = 0.005-0.07) phosphors were included for comparison. The pure phase BG phosphors with the ordered CaFe_2 O_4-type structure are obtained by annealing at 1300℃ for5 h. The phosphors with uniform particle size of 120 nm and good dispersion display typical Eu~(3+)emission with the strongest peak at 613 nm(~5 D_0→~7 F_2 transition of Eu3+) under optimal excitation band at 262 nm(CTB band). The presence of Gd~(3+) excitation bands on the PLE spectra monitoring the Eu3+emission directly proves an evidence of Gd~(3+)-Eu~(3+) energy transfer. Owing to the concentration quenching, the optimum content of Eu3+ addition is 5 at%(x = 0.05), and the quenching mechanism is determined to be the exchange reaction between Eu3+. All the BG samples have similar color coordinates and temperature of(0.64 ± 0.02, 0.36 ± 0.01) and 2000 ± 100 K,respectively. The lifetime value of BaGd_(1.9)Eu_(0.1)O_4 for 613 nm is fitted to be 2.19 ± 0.01 ms, and the Eu~(3+) concentration does not change the lifetime significantly. Owing to the Gd~(3+)-Eu~(3+) energy transfer, the luminescent intensity of the BaGd_(1.9)Eu_(0.1)O_4 phosphor is better than BY system. The BG system served as a new type of phosphor is expected to be widely used in lighting and display areas.  相似文献   

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