Eu3+在LiSrPO4中的发光及浓度猝灭机理

采用高温固相法合成了白光发光二极管用LiSrPO4:Eu3+红色荧光粉.测量了LiSrPO4:Eu3+的激发和发射光谱,结果显示材料的发射光谱为一系列尖峰,主峰位于616 nm,具有很强的红光发射;激发光谱中O2-→Eu3+的电荷迁移态CTS (220～310 nm)非常低,Eu3+的f→f (310～500 nm)跃迁吸收很强,主峰位于393 nm,与InGaN(350～410 nm)管芯匹配.比较了LiSrPO4:Eu3+与LiCaPO4:Eu3+、LiBaPO4:Eu3+发射光谱的差异,这三种晶体中Eu3+占据的格位对称性按Ca、Sr、Ba顺序逐渐增加.根据Dexter理论判定Eu3+在LiSrPO4中的浓度猝灭机理为电四极-电四极(q-q)相互作用.加入电荷补偿剂Li+、Na+和Cl 均提高了LiSrPO4:Eu3+材料的发射强度.LiSrPO4: Eu3+是一种适合白光发光二极管激发的红色荧光粉.     

新型橙红色荧光粉KNaCa2(PO4)2∶Sm3+的发光性能

利用高温固相法合成了KNaCa2(PO4)2∶Sm3+系列橙红色荧光粉,并对其发光性能进行了研究.样品的激发光谱在402 nm有很强的发射带,与近紫外LED芯片匹配.在402nm近紫外光激发下,KNaCa2(PO4)2∶Sm3+的发射光谱由3个峰组成,发射峰值位于569、601和648nm处,分别归属于Sm3+的4G5/2→ 6HJ/2(J=5,7,9)跃迁.随着Sm3+掺量的增加,样品发光强度先增强后减弱,当Sm3+掺量为0.02 mol时发光强度达到最大,浓度猝灭机理为电偶极-电偶极相互作用.分析了不同Sm3+掺杂浓度样品的荧光衰减时间,并研究了电荷补偿剂Li+对样品发光强度的影响.样品KNaCa1.96(PO4)2∶0.02Sm3+,0.02Li+发射光谱(402nm激发)的积分强度是商用红色荧光粉Y2O3∶Eu3+发射光谱(253 nm激发)的1.5倍.     

Gd~(3+)/Si~(4+)掺杂对LiZnPO_4:Eu~(3+)荧光粉发光性能的影响

采用高温固相法制备了LiZnPO4:Eu3+红色荧光粉,分别研究了Eu3+掺量、Eu3+和Gd3+共掺杂以及SiO2掺杂对材料发光性能的影响。结果表明:在395nm近紫外光激发下,发射光谱峰值位于593nm,属于Eu3+的5D0→7F1辐射跃迁;激发光谱由200~280nm的宽带和310~500nm的一系列尖峰组成,分别对应于O2–→Eu3+电荷迁移带和Eu3+的f→f能级跃迁吸收,主激发峰位于395nm左右,与近紫外发光二极管(NUV-LED)的发射光谱(360~410nm)匹配。Eu3+最佳掺杂摩尔分数为12%,超过12%后发生浓度猝灭现象,浓度猝灭机理为电多极–电多极相互作用。掺杂Gd3+、SiO2使Eu3+在593nm处的发射分别增强了107%、105%。LiZnPO4:Eu3+是适合NUV-LED管芯激发的白光发光二极管用高亮度橙红色荧光粉。     

蓝光激发的Na_2ZnSiO_4:Eu~(3+)红色荧光粉的合成及发光特性

以H3BO3作助熔剂,采用溶胶–凝胶法合成了Na2Zn Si O4:Eu3+红色荧光粉。用X射线衍射、荧光光谱分析对样品的结构及发光特性进行了表征,探讨了H3BO3助熔剂添加量和掺Eu3+量对Na2Zn Si O4:Eu3+发光性能的影响。结果表明:所得样品属于单斜晶系,样品的激发光谱主要由一系列线状谱峰组成,激发主峰为465 nm,归属于Eu3+的7F0→5D2特征跃迁。在波长为465 nm蓝光激发下发射红光,发射峰分别为578、591、613、653和701 nm,对应于Eu3+的5D0→7FJ(J=0,1,2,3,4)跃迁,发射主峰位于613 nm(5D0→7F2)处。当Eu3+和H3BO3的摩尔掺杂量分别为5%和0.8%时,样品的荧光发光强度最大。Na2Zn Si O4:Eu3+有望成为蓝光激发的白光发光二极管(w-LED)用红色荧光粉。     

Ca_(0.7)Sr_(0.3)MoO_4:Eu~(3+)红色荧光粉发光性能的改进（英文）

采用水热法制备了Ca0.70Sr0.18Mo O4:Eu0.083+,Ca0.70Sr0.18-1.5xMoO4:Eu0.083+,Lax3+与Ca0.70Sr0.18-yMo O4:Eu0.083+,La0.043+,Nay+红色荧光粉。用X射线衍射、扫描电子显微镜、荧光分光光度计对样品的物相、形貌以及发光性能进行测试和表征。结果表明:La3+离子的共掺杂可显著增强Eu3+离子的发光性能。当La3+的掺杂量为4%(摩尔分数)时,在395 nm激发下,位于616 nm处的主发射峰的相对发光强度最大。另外,电荷补偿剂Na+的引入,也明显增强了荧光粉的发光强度,荧光粉的最高发光强度是未引入Na+荧光粉的1.47倍。     

白光LED用红色发光材料CaLa_2(MoO_4)_4:Eu~(3+)的微波辅助溶胶–凝胶法合成及发光特性

以柠檬酸为络合剂,采用微波辅助溶胶–凝胶法制备了CaLa2(MoO4)4:Eu3+红色荧光粉。研究了前驱体的热分解历程,分析表征了样品的结构、形貌和发光性能。探讨了焙烧温度、Eu3+掺杂量、柠檬酸与乙二醇摩尔比和硼酸用量等对样品发光性能的影响。结果表明:前驱体经700~900℃焙烧均能得到目标产物CaLa2–x(MoO4)4:x Eu3+,样品具有白钨矿结构,属于四方晶系。样品的激发光谱在250~350 nm处有一宽吸收带,对应于Mo–O,Eu–O电荷迁移带;在395和464 nm处存在很强的吸收峰,归属于Eu3+的4f–4f跃迁。发射光谱主峰位于616 nm处,归属于Eu3+的5D0→7F2电偶极跃迁发射。前驱体经800℃焙烧所得样品发光强度最大,且发光强度随着Eu3+掺杂量的增加而增大,在x=0.2~1.0范围内未出现猝灭现象。体系中加入适量乙二醇,可以起到细化晶粒、提高粉体分散性的作用,但浓度过高则会降低样品的发光强度;助熔剂硼酸的用量对样品发光强度影响较大,当用量为3%时,样品的发光性能较好。     

碱金属、稀土元素掺杂对LiEu(SiO2)1/6W2O8荧光粉发光性能的影响

采用超声波喷雾热解法制备了红色荧光粉(Li1-aAa)Eu(SiO2)1/6W2O8,Li(Eu1-bLnb)(SiO2)1/6W2O8(A=Na,K;Ln=La,Y,Gd)。通过扫描电镜、X射线衍射、激发和发射光谱对所制样品进行分析,选择合适的实验条件可制备出颗粒呈实心球形、结晶度好、表面光滑、没有团聚现象、发光强度较高、粒径平均1μm左右且分布较窄的荧光粉样品。该类红色荧光粉激发主峰位于396 nm,次激发峰位于465 nm,发射主峰位于615 nm。随着碱金属离子半径的增加(Li 相似文献   

用于白光LED的Sr_3SiO_5:Eu~(3+)材料制备及发光特性(英文)

采用高温固相法制备了Sr3SiO5:Eu3+材料.测量了Sr3SiO5:Eu3+材料的激发与发射光谱:材料的发射光谱由576、585、611、618nm和650nm几个发射峰组成,分别对应于Eu3+的5D0→7F0、5D0→7F1、5D0→7F2、5D0→7F2和5D0→7F3辐射跃迁.监测618 nm主发射峰时所得激发光谱为一多峰宽谱,主峰分别为400nul和470nm.研究了Eu"浓度对Sr3Si05:Eu3'材料发光强度的影响,结果显示:随Etl3'浓度的增大,发光强度先增大后减小,Eu3+的摩尔分数为3%时,材料的发光强度最大,根据Dexter理论,其浓度猝灭机理为电偶极一偶极跃迁.引入电荷补偿剂Cl-、Li+、Na+和K+时,材料的发光强度均得到了提高,其中Cl-和Li+的提高幅度较明显.     

红色荧光粉LiGd(MoO4)2:Sm3+的制备与性能

利用Sm3+作为激活剂采用高温固相法制备了LiGd1-x(MoO4)2:xSm3+(x=0,0.005,0.010,0.015,0.020,0.030,0.040,0.050,0.060,0.080,0.100)系列红色荧光材料.测量了荧光粉的X射线衍射谱、激发光谱和发射光谱.在紫外光的激发下,该荧光粉的发射光谱为峰值位于564、608、648nm的三峰谱线,其中位于648nm处的红光发射最强.监测648nm发射峰得到的材料的激发光谱为一峰值位于275nm的宽谱和主峰位于363、376、404nm的线状谱线,说明该荧光粉可被紫外光和近紫外光有效地激发.研究了Sm3+掺杂浓度对LiGd(MoO4)2:Sm3+荧光粉的各发射峰发光强度的影响,得出Sm3+的最佳掺杂量(摩尔分数)为3.0％.对浓度猝灭的原因进行了探讨,结果表明该荧光粉是一种较好的用于白光LED的红色发光材料.     

Li_2ZnSiO_4∶Eu~(3+)红色荧光粉的制备及其发光性能

采用溶胶-凝胶法合成了适合于近紫外激发的Li2ZnSiO4∶Eu3+红色荧光粉,用X射线衍射、红外光谱和荧光光谱对样品进行了结构及发光性能表征。结果表明:合成样品为四方晶相Li2ZnSiO4晶体。样品的激发光谱由O2--→Eu3+电荷迁移带和Eu3+的离子特征激发峰组成。在波长为395nm的紫外激发下样品发射红光,发射主峰位于613nm,对应于Eu3+离子的5 D0→7 F2跃迁。随着Eu3+掺杂量的增加,其发光强度先增加后减小,Eu3+的最佳摩尔掺量为3.5%。     

(Ba_(1-α)Sr_α)_(4.8)(Sm_(0.7)La_(0.3))_(8.8)Ti_(18)O_(54)陶瓷的微波介电性能

采用固相合成法制备了(Ba(1-α)Srα)4.8(Sm0.7La0.3)8.8Ti18O54(α=0.1～0.5)系陶瓷,表征了该陶瓷的相组成和显微结构,测试了微波介电性能.结果表明:α=0.3时,(Ba(1-α)Srα)4.8(Sm0.7La0.3)8.8Ti18O54系陶瓷为单相的新钨青铜结构固溶体.α>0.3时,相继出现了第二相BaLa2Ti4O12和La0.66TiO2.993.随α的增加,(Ba(1-α)Srα)4.8(Sm0.7La0.3)8.8Ti18O54系陶瓷的相对介电常数(εr)先增大后有所波动,品质因数(Qf)先增大后减小,谐振频率温度系数(τf)单调减小.α=0.3时,在1 350℃烧结的陶瓷的微波介电性能最佳:εr=98.77,Qf=5184GHz,τf=10.9×10-6/℃,优于不掺杂的BaO-Sm2O3-TiO2陶瓷的.     

Fe~(3 )、Zn~(2 )、Mn~(2 )、Cu~(2 )、Ca~(2 )、Mg~(2 )等离子共存体系中Ca~(2 )、Mg~(2 )的测定

叙述了Fe3 、Zn2 、Mn2 、Cu2 、Ca2 、Mg2 等离子共存体系中采用六次甲基四胺 -铜试剂沉淀除去Fe3 、Zn2 、Mn2 、Cu2 等干扰离子 ,用EDTA滴定钙镁的方法 ,该方法钙的回收率在 99.7%～ 10 0 .3 % ;镁的回收率在 10 0 .0 %～ 10 0 .4% ,标准偏差为 0 .0 2 2。     

(K_(0.485)Na_(0.485)Li_(0.03))NbO_3-Pb(Zr_(0.53)Ti_(0.47))O_3压电陶瓷的压电性能与微观结构

采用传统电子陶瓷制备技术和工业原料制备了新型(1-x)(K0.485Na0.485>Li0.03)NbO3-Pb(Zr0.53Ti0.47)O3少铅压电陶瓷,研究了该体系陶瓷的压电性能及微观结构.X射线衍射分析表明:在1250℃烧结3h的条件下,所有陶瓷样品都具有纯的钙钛矿结构和高致密性,并且在室温下形成了正交相和四方相共存的结构.x=0.75时,陶瓷的压电性能达到最佳:压电常数d33=363 pC/N,机电耦合系数kp=63%,相对介电常数εr=1 590,介质损耗tanδ=1.70%.     

Adhesion of calcium phosphate coatings on polyethylene (PE), polystyrene (PS), poly(tetrafluoroethylene) (PTFE), poly(dimethylsiloxane) (PDMS) and poly-L-lactic acid (PLLA)

Calcium phosphate (CaP) coatings can be applied to improve the biological performance of polymeric medical implants. For clinical applications, a strong adhesion of the coating to the polymeric substrate is important. Therefore, the adhesion of rf magnetron-sputter-deposited CaP coatings on five polymers was studied: polyethylene (PE), polystyrene (PS), poly(tetrafluoroethylene) (PTFE), poly-L-lactic acid (PLLA) and poly(dimethylsiloxane) (PDMS). To influence the adhesion, the interface was varied in six different ways, e. g. by a plasma or ion-beam pretreatment, or by using a Ti interlayer. The adhesion was determined by using scratch, tensile and 180^° bend tests. Especially the polymers PE and PS needed a bombardment by energetic particles prior to or during coating deposition, to enable the formation of chemical bonds between the coating and the polymer, which gave adhesion. On PLLA and PDMS, being oxygen containing polymers, it was easier to establish a strong interface. An overtreatment of the polymeric substrates gave worse adhesion, probably due to the formation of weak low molecular weight (LMW) layers on the polymer. On PTFE, the use of a Ti interlayer was necessary to prevent the PTFE from UV degradation during coating deposition, as this caused cohesive failure within the PTFE. The results showed that each polymer requires a different approach for obtaining optimal adhesion. The observed adhesion could often be explained in the terms of processes occurred during the pretreatment of the polymers or the deposition of the coating.     

Ba(Zr_(0.055)Ti_(0.945))O_3含量对[(Na_(0.80)K_(0.16)Li_(0.04))_(0.5)Bi_(0.5)]TiO_3陶瓷性能的影响

系统研究(1-y)[(Na0.80K0.16Li0.04)0.5Bi0.5]TiO3-yBa(Zr0.055Ti0.945)O3无铅压电陶瓷,获得压电应变常数高达185pC/N的0.94[(Na0.80K0.16Li0.04)0.5Bi0.5]-TiO3-0.06Ba(Zr0.055Ti0.945)O3压电陶瓷。样品的晶体结构为三方相、四方相共存,处于准同型相界(morphotropic phase boundary,MPB)附近。该类陶瓷室温MPB的摩尔(下同)含量为0.050y0.065。样品y=0.060在40°左右的(003)、(021)双峰与46.5°左右的(002)、(200)双峰分裂最明显。随着Ba(Zr0.055Ti0.945)O3含量的增加,铁电相-反铁电相相变温度(θd)升高、反铁电相-顺电相相变温度(θm)降低;θd和θm的温差越来越小,材料的弛豫性逐渐降低。     

Ternary Complexes of cis-(NH(3))(2)PtCl(2) (cis-DDP) With Guanosine (guo), Cytidine (cyd) and the Aminoacids Glycine (gly), L-Alanine (ala), L-2-Aminobutyric Acid (2-aba), L-Norvaline (nval) and L-Norleucine (nleu)

The ternary complexes of formulae cis-[(NH(3))(2)Pt(nucl)(amac)]NO(3), where nucl = guo and cyd (guanosine and cytidine) and amac = the deprotonated aminoacids glycine (gly), L-alanine (ala), L-2-aminobutyric acid (2-aba), L-norvaline (nval) and L-norleucine (nleu), were prepared from the reactions of the binary chelated ones cis-[(NH(3))(2)Pt(nucl)(amac)]NO(3) with the nucleosides.They were characterized by (1)H, (13)C and (195)Pt NMR and IR spectra, together with elemental analysis and conductivity measurements. The aminoacids coordinate with Pt(II) in the ternary complexes with their terminal -NH(2) groups, guo through N(7) and cyd through N(3). Ligand-ligand hydrophobic interactions were also observed in the ternary complexes and were stronger with longer aliphatic chains of the aminoacids. The (3)E sugar conformation increased by 5-7% in the ternary systems, as compared to the free nucleosides, while the percentage of the gg conformation remained almost constant and the one of the anti conformation of the sugar increased also slightly. Finally, the h conformer around the C(alpha)-C(beta) bonds of the aminoacids reached a maximum in the binary systems and decreased again considerably in the ternary ones.     

La掺杂(Na_(0.5)Bi_(0.5))_(0.82)(K_(0.5)Bi_(0.5))_(0.18)TiO_3系统无铅压电陶瓷的制备工艺探讨

采用传统陶瓷工艺,研究了制备[(Na0.5Bi0.5)0.82(K0.5Bi0.5)0.18]1-xLaxTiO3(x=0.00,0.01,0.03,0.05,0.10)无铅压电陶瓷的工艺条件对陶瓷的物相组成、显微结构和压电性能的影响。利用XRD、SEM等技术分析结果表明,合成温度的提高有利于主晶相的形成,且此系统烧成温度范围较窄,故需控制在合适的烧成温度下才能得到高致密度的陶瓷。同时,研究了极化工艺条件对材料压电性能的影响,结果表明,提高极化电场强度、控制适当的极化温度有利于提高材料的压电性能。     

Infrared Study of Er(3+)/Yb(3+) Co-Doped GeO(2)-PbO-Bi(2)O(3) Glass

Heavy metal oxide glasses, containing bismuth and/or lead in their glass structure are new alternatives for rare eart (RE) doped hosts. Hence, the study of the structure of these vitreous systems is of great interest for science and technology. In this research work, GeO(2)-PbO-Bi(2)O(3) glass host doped with Er(3+)/Yb(3+) ions was synthesized by a conventional melt quenching method. The Fourier transform infrared (FTIR) results showed that PbO and Bi(2)O(3) participate with PbO(4) tetragonal pyramids and strongly distort BiO(6) octahedral units in the glass network, which subsequently act as modifiers in glass structure. These results also confirmed the existence of both four and six coordination of germanium oxide in glass matrix.