基于CaBa_2(BO_3)_2中的Ce~(3+)→Tb~(3+)能量传递及光谱特性

采用高温固相法合成了Ce3+,Tb3+掺杂激活的CaBa2(BO3)2荧光粉,并对其发光特性进行了研究。观察到CaBa2(BO3)2中Ce3+对Tb3+发光的敏化现象。在367 nm紫外光激发下,单掺Tb3+时CaBa2(BO3)2不发光。当Ce3+和Tb3+共掺时,出现Tb3+的发射峰,样品发绿光,表明Ce3+对Tb3+的发光有很强的敏化作用。根据Forster-Dexter理论,分析Ce3+和Tb3+的能量传递过程,还证明在CaBa2(BO3)2:Ce3+,Tb3+中Ce3+对Tb3+的能量传递属于共振能量传递。     

紫外激发Sr1-x-yMgP2O7:xCe3+,yTb3+荧光粉的发光特性及能量传递

采用高温固相法合成了Sr1-x-yMgP2O7:xCe3+,yTb3+荧光粉.研究了荧光粉的晶体结构、发光特性、荧光寿命、能量传递机理和荧光粉的热稳定性.研究结果表明:在SrMgP2O7基质中,Ce3+的发射峰值为398nm,Tb3+的主发射峰值为545nm,它们分别属于5d-4f跃迁和5D4→7F5跃迁.Ce3+和Tb3+共掺时,Ce3+和Tb3+通过电偶极子-电偶极子相互作用发生能量传递,能量传递的临界距离为0.614nm.通过计算得到单掺杂Ce3+、Tb3+时热猝灭过程的激活能分别为0.122和0.111eV,Tb3+离子的发光热稳定性比Ce3+离子的好.     

稀土亚磷酸盐GdxTb2-x（HPO3）3（H2O）2（0≤x≤2）的微波合成、表征与性质研究

利用微波辅助合成法,成功地合成出一系列新颖的稀土亚磷酸盐GdxTb2-x(HPO3)3(H2O)2(0≤x≤2).X-射线粉末衍射分析结果表明,它们为同构的化合物.对Gd2(HPO3)3(H2O)2进行X-射线单晶衍射分析得出,该化合物结晶于P21/c空间群,晶胞参数为a=6.9124(6),b=12.8891(12),c=12.3692(11),β=100.1520(10)°.Gd2(HPO3)3(H2O)2是由GdO7多面体,GdO8多面体和[HPO3]假四面体通过共用氧原子相互连接而成的三维骨架.Gd2(HPO3)3(H2O)2和Tb2(HPO3)3(H2O)2的荧光光谱分别显示Gd3+和Tb3+的特征发光.Gd/Tb掺杂的样品中存在Gd3+-Tb3+的能量传递,它们的发光显示Tb3+的绿光发射(5D4→7F3-6),并且5D4→7F3跃迁的强度随着Tb3+掺杂量的增大而增强,这表明Gd2(HPO3)3(H2O)2引入不同浓度的发光中心Tb3+之后可以作为绿光发光材料.磁性研究表明,Gd2(HPO3)3(H2O)2中存在极弱的反铁磁相互作用.     

CaO-SiO2-B2O3:Sm2O3玻璃的合成及Sm3+发光性质研究

用常规的高温合成法合成了CaO-SiO2-B2O3Sm2O3玻璃, 探讨了玻璃的最佳合成温度、玻璃的吸收光谱, 并研究了其发光性质. 在CaO-SiO2-B2O3Sm2O3玻璃体系中观察到了Sm3+的发射光谱. 样品的发射光谱有3个主要荧光发射峰, 峰值波长分别为568, 605, 650 nm, 其中最强峰为605 nm,可见发射起源于Sm3+离子4f电子的f-f跃迁. 其中568 nm对应于4G5/2→6H5/2跃迁、 605 nm对应于4G5/2→6H7/2跃迁、 650 nm对应于4G5/2→6H9/2跃迁, 光谱性质表明这种玻璃体系能够把太阳光中的紫外光转换成红光, 从而增强红光的发射强度. 可以利用这些玻璃的发光性质来制备农用转光玻璃.     

Sr2MgSi2O7∶Tb3+，Li+荧光粉的合成和发光机理

采用高温固相法合成Sr2-mMg1-nSi2O7∶mTb3+,nLi+(m=0.03~0.50,n=m)系列荧光粉。使用X射线衍射仪和荧光光谱仪对样品的物相和发光性质进行了表征。在377 nm紫外光激发下,荧光粉的发射光谱呈多谱带发射,主峰位于490 nm,542 nm,590 nm和613 nm处,分别对应于Tb3+的5D4→7FJ(J=6,5,4,3)跃迁发射。调节Tb3+离子掺杂浓度,可实现荧光粉的发光颜色从蓝到白、黄、绿的可调发射;名义组成为Sr1.95Mg0.95Si2O7∶0.05Tb3+,0.05Li+的荧光粉在紫外光(377 nm)激发下发白光,其色坐标(0.322,0.317)接近纯白光(0.33,0.33),是一种潜在的LED用单基质白光荧光粉。     

铈、钐掺杂YAG微晶玻璃制备及光谱性能

以Y2O3-A l2O3-S iO2-L i2O-K2O-Na2O玻璃作为Ce,Sm掺杂基质玻璃,制备出白光LED用YAG:Ce和YAG:Ce,Sm微晶玻璃。利用X射线衍射、荧光光度计对微晶玻璃的晶相、光谱性能及荧光寿命进行了研究。结果表明:掺杂铈或铈钐共掺杂基质玻璃在1400℃热处理得到的几乎是纯YAG晶相;并且YAG:Ce和YAG:Ce,Sm微晶玻璃在454 nm有特征激发峰,说明它们能被蓝光芯片有效激发;在蓝光芯片激发下,YAG:Ce微晶玻璃在480~700 nm产生有效发射,发射光谱中心波长531 nm,同时铈钐共掺微晶玻璃在566,602,615,650 nm都有窄的发射峰,可以提高LED s的显色性、降低色温;此外,浓度掺杂实验表明钐的较好掺杂浓度范围是Ce:Sm为10∶2~10∶10;YAG:Ce和YAG:Ce,Sm微晶玻璃的荧光衰减曲线表明,YAG:Ce微晶玻璃的荧光寿命要长于YAG:Ce,Sm微晶玻璃。     

Ce4+和Eu3+共掺杂的Ca2SnO4发光材料的合成与光谱特性

利用高温固相反应法合成了Ce4 和Eu3 共掺杂的Ca2-xEuxSn1-yCeyO4样品,并对其结构和发光特性进行了研究。X射线衍射结果显示,在Ca2SnO4中同时掺入Ce4 和Eu3 离子没有改变其晶体结构。Ca2-xEuxSn1-yCeyO4样品的发射光谱随Eu3 掺杂浓度产生很大变化,当Eu3 掺杂浓度低时,样品中同时存在着Ce4 -O2-的蓝光发射和Eu3 的红光发射;当Eu3 掺杂浓度较高时,样品呈现出Eu3 离子的红光发射。Ce4 -O2-蓝色发光的寿命约为81μs,其能量来源于O2-和Ce4 离子间的电荷迁移吸收;而Eu3 红色发光的寿命约为830μs,其能量来源于O2-和Eu3 离子间的电荷迁移吸收。Eu3 -O2-键比Ce4 -O2-键更容易吸收紫外光,两者之间没有能量传递现象。     

CaO-SiO_2-B_2O_3∶Sm_2O_3玻璃的合成及Sm~(3 )发光性质研究

用常规的高温合成法合成了CaO-SiO2-B2O3∶Sm2O3玻璃,探讨了玻璃的最佳合成温度、玻璃的吸收光谱,并研究了其发光性质。在CaO-SiO2-B2O3∶Sm2O3玻璃体系中观察到了Sm3 的发射光谱。样品的发射光谱有3个主要荧光发射峰,峰值波长分别为568,605,650nm,其中最强峰为605nm,可见发射起源于Sm3 离子4f电子的f-f跃迁。其中568nm对应于4G5/2→6H5/2跃迁、605nm对应于4G5/2→6H7/2跃迁、650nm对应于4G5/2→6H9/2跃迁,光谱性质表明这种玻璃体系能够把太阳光中的紫外光转换成红光,从而增强红光的发射强度。可以利用这些玻璃的发光性质来制备农用转光玻璃。     

KSrBP2O8:RE(RE=Eu2+,Tb3+,Eu3+)荧光粉的制备与发光性能研究

采用高温固相反应法制备了KSrBP2O8:RE(RE=Eu2+,Tb3+,Eu3+)系列荧光粉。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:稀土离子的掺入没有改变荧光粉的主晶相。利用荧光光谱仪对样品的发光性能进行了测试,发现在近紫外光激发下掺杂Eu2+离子的样品具有宽带发射峰,最强发射位于450 nm左右,对应于Eu2+离子的4f65d1→4f7辐射跃迁。随着Eu2+掺杂量的增加,发射光从蓝光逐渐转变到蓝白光。另外,KSrBP2O8:Tb3+和KSrBP2O8:Eu3+能够在近紫外光激发下分别发射出绿光和红光,其最佳掺杂浓度分别为0.04%和0.08%(摩尔分数)。     

YAG:Ce,Mn微晶玻璃的制备及光谱性能研究

由于YAG:Ce微晶玻璃缺乏红色发光成分,导致其封装的白光LED显色指数低.以Y2O3-Al2 O3-SiO2-Li2O作为Ce,Mn掺杂的基质,制备了可提高显色指数的白光LED用YAG:Ce,Mn微晶玻璃.通过XRD测试、荧光测试和电光源测试表征了玻璃的晶相结构、光谱性能及荧光寿命,研究了Mn2+对YAG:Ce微晶玻璃发光的影响,并对其增红机制进行了探讨.结果表明:基玻璃在1400℃热处理可析出纯YAG晶相;YAG:Ce,Mn微晶玻璃在460 nm光激发下,在530 nm处有Ce3+的特征发射峰,由于Ce3+-Mn2+之间的能量传递,在585 nm处有Mn2的特征发射峰,从而使得YAG:Ce,Mn微晶玻璃的发光峰比YAG:Ce微晶玻璃的发光峰向红光方向宽化,有效地提高了白光LED的显色性能.     

Ce3+,Tb3+,Eu3+共掺杂Sr2MgSi2O7体系的白色发光和能量传递机理

通过正交试验,采用高温固相法制备了Sr2-x-y-zMgSi2O7∶xCe3+,yTb3+,zEu3+系列样品.使用X射线衍射仪和荧光光谱仪表征了样品的物相和发光性质,并讨论了Ce3+-Tb3+-Eu3+共掺杂Sr2MgSi2O7体系中的能量传递过程.实验结果表明,在327 nm波长激发下,所合成荧光粉的发射峰主要位于387 nm(蓝紫)、542nm(绿)和611 nm(红)处;分别以387,542和611 nm为监控波长,所得激发光谱显示荧光粉在327 nm处有最好的激发.在327 nm光激发下,系列样品发光进入白光区.最优化的荧光粉为Sr1.91MgSi2O7∶0.01Ce3+,0.05Tb3+,0.03Eu3+,其色坐标为(0.337,0.313),是一种潜在的发光二极管(LED)用白色荧光粉.     

Er3+和Ce3+/Ce4+掺杂β-BaB2O4纳米棒的制备、结构与发光性质

以Ba(NO3)2、NaBH4、Er2O3和CeO2为原料, 在十六烷基三甲基溴化铵(CTAB)表面活性剂辅助下, 采用水热法制备了β-BaB2O4 (β-BBO)纳米棒, 稀土离子Er3+单掺杂的β-BBO(β-BBO:Er3+)及Er3+和Ce3+/Ce4+共掺杂的β-BBO(β-BBO:Er3+/Ce3+/Ce4+)纳米棒. 通过X射线粉末衍射(XRD)、傅里叶变换红外(FTIR)光谱、拉曼光谱、扫描电子显微镜(SEM)、透射电子显微镜(TEM)、X射线光电子能谱(XPS)和光致发光(PL)光谱分别对样品的物相、结构、形貌、成分及光致发光性质进行了表征. 研究结果表明: 微量稀土离子掺杂并不改变β-BBO的结构, 制得的纳米棒尺寸均匀, 长度在200-500 nm 之间, 直径在10-20 nm 之间; β-BBO:Er3+和β-BBO:Er3+/Ce3+/Ce4+纳米棒在400nm光激发下, 在可见光范围内都观察到中心波长为515和542 nm的绿光. 对发光机理的初步研究表明: 发光分别对应于Er3+的2H11/2→4I15/2, 4S3/2→4I15/2跃迁, 铈离子以Ce3+和Ce4+两种形式存在于体系中, Ce3+对Er3+起敏化作用, 可以显著增强β-BBO:Er3+/Ce3+/Ce4+纳米棒的发光强度, 存在Ce3+→Er3+的能量传递过程.     

磷灰石结构荧光粉Ba10(PO4)6F2:Ce3+,Tb3+的合成、发光和能量传递

采用高温固相法合成了系列Ce~(3+)和Ce~(3+)/Tb~(3+)激活的具有磷灰石结构荧光粉Ba_(10)(PO_4)_6F_2。用X射线衍射(XRD)、扫描电镜(SEM)、激发和发射(PLE和PL)光谱对样品进行了表征分析。研究结果表明:所合成的荧光粉Ba_(10)(PO_4)_6F_2∶Ce~(3+),Tb~(3+)具有氟磷灰石结构,样品微观呈现不规则形貌。荧光粉Ba10-x(PO4)6F2∶x Ce~(3+)的相对发射强度随着x增加而增强,当x=0.09时,荧光强度达到最大。荧光粉Ba_(10)(PO_4)_6F_2∶Ce~(3+),Tb~(3+)的激发光谱为240～330 nm的宽带,发射光谱呈现出Ce~(3+)的5d→4f跃迁紫外光(335和358 nm)发射和Tb~(3+)的4f→4f跃迁绿光(542 nm)发射。光谱特性表明,发光过程中存在Ce~(3+)→Tb~(3+)能量传递,能量传递效率可以达到60%。计算Ce~(3+)和Tb~(3+)的临界距离为0.79 nm,能量传递机理是偶极-偶极交互作用。此外,详细论述了Ce~(3+)和Tb~(3+)之间的能量传递和发光的过程。通过调节Tb~(3+)的掺杂浓度,对荧光粉发光色坐标与Tb~(3+)的掺杂浓度之间的关系也进行了研究,随着Tb~(3+)的掺杂量从0增加0.52,荧光粉Ba_(10)(PO_4)_6F_2∶Ce~(3+),Tb~(3+)的发射光谱色坐标可以从(0.149 4,0.045 1)蓝色区变化到(0.280 1,0.585 3)绿色区。     

Ce3+和Tb3+掺杂的稀土硼酸盐玻璃的发光性质

报道Ｃｅ＾３＋和Ｔｂ＾３＋掺杂的硼酸盐玻璃的合成及该系列玻璃的激发和发射光谱性质。在紫外光激发下,玻璃中的Ｃｅ＾３＋发射蓝紫光,Ｔｂ＾３＋发射有特征的绿光,在Ｃｅ＾３＋和Ｔｂ＾３＋共掺杂的体系中,可观察到Ｃｅ＾３＋强烈敏化Ｔｂ＾３＋发光的现象。分析表明,Ｃｅ＾３＋和Ｔｂ＾３＋之间存在辐射能量传递稿铲无辐射能量传递。     

A novel strategy for controllable emissions from Eu3+ or Sm3+ ions co-doped SrY2O4:Tb3+ phosphors

Trivalent rare-earth (RE) ions (Eu(3+), Tb(3+) and Sm(3+)) activated multicolor emitting SrY(2)O(4) phosphors were synthesized by a sol-gel process. The structural and morphological studies were performed by the measurements of X-ray diffraction profiles and scanning electron microscope (SEM) images. The pure phase of SrY(2)O(4) appeared after annealing at 1300 °C and the doping of RE ions did not show any effect on the structural properties. From the SEM images, the closely packed particles were observed due to the roughness of each particle tip. The photoluminescence (PL) analysis of individual RE ions activated SrY(2)O(4) phosphors exhibits excellent emission properties in their respective regions. The Eu(3+) co-activated SrY(2)O(4):Tb(3+) phosphor creates different emissions by controlling the energy transfer from Tb(3+) to Eu(3+) ions. Based on the excitation wavelengths, multiple (green, orange and white) emissions were obtained by Sm(3+) ions co-activated with SrY(2)O(4):Tb(3+) phosphors. The decay measurements were carried out for analyzing the energy transfer efficiency and the possible ways of energy transfer from donor to acceptor. The cathodoluminescence properties of these phosphors show similar behavior as PL properties except the energy transfer process. The obtained results indicated that the energy transfer process was quite opposite to the PL properties. The calculated CIE chromaticity coordinates of RE ions activated SrY(2)O(4) phosphors confirmed the red, green, orange and white emissions.     

绿色荧光粉Ba2-xB2O5:xTb3+的制备及发光性能研究

采用高温固相法合成了Ba2-xB2O5:xTb3+绿色荧光粉。XRD图谱表明合成物质为纯相的Ba2B2O5晶体。该样品在256 nm(4f8→4f75d1)处有最强激发;有4个发射峰,分别位于489 nm(5D4→7F6),545 nm(5D4→7F5),585 nm(5D4→7F4)和622 nm(5D4→7F3);其中在545 nm处有最强发射。随着Tb3+掺杂浓度的不同,激发峰与发射峰的强度先增大后减小,当x=0.7时最佳。研究了电荷补偿剂Na+对发光性能的影响,样品的发射光谱强度随Na+掺杂浓度的增大而增大,当掺杂浓度达到或超过Tb3+浓度后发射光谱强度下降。     

A family of three-dimensional 3d-4f and 4d-4f heterometallic coordination polymers based on mixed isonicotinate and 2-sulfobenzoate ligands: syntheses, structures and photoluminescent properties

Hydrothermal reactions of isonicotinic acid (Hina), 2-sulfobenzoic acid (H(2)sba), d-block metal salts and lanthanide oxides/hydroxides yielded 17 three-dimensional (3D) 3d-4f and 4d-4f heterometallic coordination polymers (HCPs). They are formulated as [LaAg(sba)(ina)(2)](n) (1), [Ln(2)Ag(2)(sba)(2)(ina)(4)(H(2)O)(2)](n) [Ln = Pr (2), Nd (3), Sm (4), Eu (5), Gd (6), Tb (7), Dy (8), Ho (9), Er (10)] and [Ln(2)Cu(2)(sba)(2)(ina)(4)(H(2)O)(2)](n) [Ln = La (11), Pr (12), Nd (13), Sm (14), Eu (15), Gd (16), Tb (17)]. Their structures were characterized by single crystal X-ray diffraction, powder X-ray diffraction (XRD), infrared (IR) spectroscopy, elemental analysis (EA), and thermogravimetric analysis (TGA). It reveals that they represent two structural types of 3D HCPs. Furthermore, the investigations of their solid-state photoluminescent (PL) property demonstrate the extraordinary emission behaviors. HCP 1(La-Ag) exhibits tunable blue-to-green PL emissions by variation of excitation light. HCPs 6(Gd-Ag), 11(La-Cu), 12(Pr-Cu) and 16(Gd-Cu) show d(10)-metal-based ligand-to-metal charge transfer (LMCT) or metal-to-ligand charge transfer (MLCT) emissions. HCPs 3(Nd-Ag), 4(Sm-Ag), 5(Eu-Ag), 7(Tb-Ag), 8(Dy-Ag), 13(Nd-Cu), 14(Sm-Cu), 15(Eu-Cu) and 17(Tb-Cu) display characteristic PL emissions of the corresponding Ln(III) ions, while both d(10)-metal-based and 4f-metal-centered emissions are observed in the emission spectra of 4(Sm-Ag), 8(Dy-Ag), 14(Sm-Cu) and 17(Tb-Cu).     

Synthesis and Luminescent Properties of Nano-scale Y2Si2O7:Re3+ (Re=Eu,Tb) Phosphors via Sol-Gel Method

By using metal nitrates as starting materials and citric acid as a complexing agent, Y2Si2O7:Re3+ (Re=Eu, Tb) phosphors were prepared by a sol-gel method. X-ray diffraction was employed to characterize the resulting samples. The results of XRD indicate that the ff-Y2Si2O7 nanocrystal with size of 27 nm is obtained at 1000 oC and the doping ion content does not influence the structure. The excitation spectra in the UV and VUV ranges and the emission spectra of Re3+ doped samples were measured. The excitation spectra in the VUV range is due to absorption of host, that in the UV range is ascribed to absorption transitions from 4f to 5d state of the Tb3+ and the charge transfer in the Eu3+-O2- bond. The spectral energy distribution of the Tb3+ emission depends strongly on the Tb3+ concentration. The dependence of photoluminescence intensity on Re3+ concentration is also discussed in detail. The fluorescent decay curves at room temperature were measured and analyzed.     

激活CaO-MgO-SiO_2长余辉玻璃发光性质

报道了一种新型的Eu~(2+)离子激活硅酸盐玻璃,该玻璃组成为2CaO-MgO-3SiO_2-0.015Eu_2O_3(CMSE)。通过透射光谱、稳态荧光光谱、余辉光谱和热释光等技术手段对CMSE的发光性质进行了深入研究。研究发现CMSE可以被紫光和近紫外光激发,获得黄色长余辉发光。热释光曲线的分析表明,CMSE的长余辉性质主要来自于玻璃基质中陷阱深度为0.83 e V左右的定域能级。研究认为对CMSE发光性质的研究有利于开发新型稀土离子激活近紫外激发LED用硅酸盐玻璃发光材料。     

Study of the luminescence properties of a novel rare earth complex Tb(DPC)22H2O

Rare earth complex Tb(DPC)₂2H₂O was synthesized by introducing Pyridine-2,6-dicarboxylic acid(H₂DPC) as the ligand and characterized by UV, fluorescent and infrared spectra as well as elemental analysis. The complex exhibited ligand-sensitized green emission, and it has the higher sensitized luminescent efficiency and longer lifetime. The effect and mechanism of the ligand (H₂DPC) on the luminescence properties of terbium complex was discussed. In device ITO/PVK/Tb(DPC)₂2H₂O/Al, Tb³⁺ may be excited by intramolecular energy transfer from ligand as observed by electroluminescence. The main emitting peak at 545 nm can be attributed to the transition of ⁵D₄→⁷F₅ of Tb³⁺ ion and this process results in the enhancement of green emission from electroluminescence device.