氟化镁锶中铕和铽的电荷迁移及其平衡解析

在氩气氛中，合成了SrMgF4：xEu，yTb复合组化物磷光体．该体系中Eu3 和Eu2 共存．随共掺入Tb浓度的增加，Eu3 的荧光发射强度降低，Eu2 的发光增强；并且Eu2 的ESR信号增强．认为Eu3 和Tb3 之间存在电荷迁移．即Eu3 ＋Tb3 →Eu2 ＋Tb4 .通过半定量手段研究了这一电荷迁移反应的平衡常数     

CaS:Ce~(3+)荧光粉中的电荷迁移态光谱

本文报道了CaS:Ce~(3+),Na~+和CaS:Ce~(3+)X~-(X=F、Cl、Br)荧光粉的220nm附近的激发光谱,它是由S~(2-)的3P~6电子迁移到Ce~(3+)的4f轨道所致的电荷迁移态激发。以卤素为共激活剂时,对激发带向低波数的移动作了分析。     

利用电荷迁移反应分光光度法测定头孢唑林钠的研究

研究了π受体试剂四氯苯醌与头孢唑林钠的电荷迁移反应。发现在乙酰丙酮乙二醇聚乙二醇２００体系中，两者形成稳定的橙色络合物。络合物比为１∶１，λｍａｘ＝４５２ｎｍ。药物质量浓度在２０～８００ｍｇ／Ｌ范围呈线性。用该法测量试样含量与药典法一致。相对标准偏差１．０％（ｎ＝１０），加标回收率９７％以上。     

准一维有机电荷迁移晶体电导率和温度的关系

在有机电荷迁移晶体中,有一类是由荷正电的施体分子柱与荷负电的受体分子柱交错平行排列而成,如TTF-TCNQ,因为这类晶体具有很强的各向异性,表现为准一维导体.实验得到,在T_P相似文献   

无机晶体中Zr4+电荷迁移能与基质平均能隙关系

电荷迁移跃迁是指电子在配体的低能轨道受激往金属离子的高能轨道发生的跃迁[1].其光谱位置较高,一般位于真空紫外(VUV)区域,可以有效地吸收200 nm左右的激发能量,因此,对真空紫外发光材料起着非常重要的作用翻[2].     

N-甲基-2-(4'-N-乙基咔唑基)-[60]富勒烯吡咯烷及其衍生物的合成, 电荷分离态特征

通过1,3-偶极环加成方法在微波照射下合成了N-甲基-2-(4'-N-乙基咔唑基)-富勒烯吡咯烷(C₆₀-Cz)和N-甲基-2- (4'-N,N-二苯基氨基)-富勒烯吡咯烷(C₆₀-TPA), 用质谱, ¹H NMR, IR等对其结构进行了表征. 用激光光解时间分辨瞬态谱研究了N-甲基-2-(4'-N-乙基咔唑基)-富勒烯吡咯烷的分子内电荷转移过程, 在近红外区观测到了长寿命电荷分离态C₆₀^•--C_Z^•+的存在, 其寿命为0.28 μs. 运用Gaussian 98量子化学程序包, 利用密度泛函的方法对N-甲基-2-(4'-N,N-二苯基氨基)-富勒烯吡咯烷几何构型进行了优化, 并在优化基础上用ZINDO方法计算了化合物C₆₀-TPA的电子光谱, 计算结果表明, 光谱吸收峰在440 nm, 与实验值433 nm基本一致.     

ZSM－5沸石中V的还原性能

用ＴＰＲ并结合ＸＲＤ、ＥＳＲ和ＸＰＳ等测试手段研究了Ｖ（Ⅳ，Ⅴ）－ＺＳＭ－５、Ｖ２Ｏ５－／ＺＳＭ－５（分别用浸渍法和机械混合法制备）及Ｖ２Ｏ５样品的还原性能，获得了还原过程中物相及钒离子价态变化的信息，发现分散在分子筛表面上的Ｖ（Ⅴ）还原温度比Ｖ２Ｏ５低，而位于ＺＳＭ－５骨架上的Ｖ（Ⅴ）却比Ｖ２Ｏ５更难还原。高于１２００Ｋ骨架Ｖ才开始还原；高于１３７０Ｋ，Ｖ－ＺＳＭ－５分子筛开始解体并转变成方英石结构，从骨架中析出的Ｖ完全还原成低价态。     

ZSM-5沸石中V的还原性能

用TPR并结合XRD、ESR和XPS等测试手段研究了V(Ⅳ,Ⅴ)-ZSM-5、V₂O₅-/ZSM-5(分别用浸渍法和机械混合法制备)及V₂O₅样品的还原性能,获得了还原过程中物相及钒离子价态变化的信息,发现分散在分子筛表面上的V(Ⅴ)还原温度比V₂O₅低,而位于ZSM-5骨架上的V(Ⅴ)却比V₂O₅更难还原。高于1200K骨架V才开始还原;高于1370K,V-ZSM-5分子筛开始解体并转变成方英石结构,从骨架中析出的V完全还原成低价态。     

MMgF4(M=Ca,Sr, Ba)体系中Eu和Tb的电荷迁移

于不同气流中, 合成了MMgF4:xEu,yTb复合氟化物磷光体。该体系中Eu^3^+和Eu^2^+共存。Tb的存在影响Eu的价态存在形式。ESR测试表明, 随Tb的掺入浓度增加, Eu^2^+的浓度呈规律性变化。随Eu的掺入, 样品的XPS谱中出现了四价铽的Tb3d5/2特征伴峰。认为Eu^3^+和Tb^3^+之间存在电荷迁移平衡。即Eu^3^++Tb^3^+=Eu^2^++Tb^4^+。通过半定量手段研究了SrMgF4中这一衡的平衡常数。     

铕和铽与3,4-呋喃二甲酸双核配合物的合成、表征及其晶体结构

本文首次合成了铕(Ⅲ)和铽(Ⅲ)与3,4-呋喃二甲酸配合物,研究了它们的IR、DTA、TG、DTG和荧光光谱等性质,并完成了单晶的晶体分析。结果表明,配合物为〔Ln·HL_2(H_2O)_2〕_2·2H_2O(Ln=Eu(Ⅲ),Tb(Ⅲ);H_2L=3,4-呋喃二甲酸),属单斜晶系,P2/c空间群,Z=2,晶胞参数对铕和铽配合物分别为α=10.842(1),10.801(4);b=8.725(2),8.664(2);c=16.366(4),16.308(6)A;β=93.50(1),93.67(3)°;V=1545.3(5),1523.0(8)A~3。     

Photoluminescence and energy transfer in Tb/Mn co-doped ZnAl2O4 glass ceramics

We report on Tb³⁺ as efficient sensitizer for red photoemission from Mn²⁺-centers in ZnO-B₂O₃-Al₂O₃-Si₂O-Na₂O-SrO glasses and corresponding gahnite glass ceramics. In comparison to singly or co-doped glasses, the glass ceramics exhibit significantly increased emission intensity. Structural considerations, ESR, and dynamic luminescence spectroscopy indicate partial incorporation of Mn²⁺ as well as Tb³⁺ into the crystalline phase, the former on octahedral Zn²⁺-sites. Interionic distance and charge transfer probability between both species depend on crystallization conditions. This enables control of the energy transfer process and, hence, tunability of the color of photoemission by simultaneous emission from Tb³⁺ and Mn²⁺ centers. Concentration quenching in Mn²⁺-singly doped materials was found at a critical dopant concentration of about 1.0 mol%. The energy transfer process was studied in detail by dynamic as well as static luminescence spectroscopy. Spectroscopic results suggest the application of the studied materials as single or dual-mode emitting phosphor for luminescent lighting.     

BaLiF3∶Eu,Gd中Gd3+→Eu2+的能量传递

研究了BaLiF3中Gd3+和Eu2+的光谱性质及Gd3+对Eu2+的能量传递过程,讨论了传递机理.Gd3+的含量(物质的量分数)为0.3%时,传递效率最高,传递几率PSA＝1.35×105 s-1.当Gd3+的含量高于0.3%时,由于Gd3+和Eu2+竞争吸收Gd3+占优势,增加Gd3+含量,竞争吸收比相应增加,Eu2+自身吸收光子数目减少,发射强度降低.     

Photoluminescence of Ce, Pr and Tb activated Sr3Ln(PO4)3 under VUV-UV excitation

The spectroscopic properties in VUV-Vis range for the eulytite structural phosphors Sr₃Gd(PO₄)₃:Ln³⁺ (Ln³⁺=Ce³⁺, Pr³⁺, Tb³⁺), Sr₃Ce(PO₄)₃, Sr₃Gd(PO₄)₃ and Sr₃Tb(PO₄)₃ were investigated. The bands near 170 nm in VUV excitation spectra are assumed to connect with the host lattices related absorption. The f-d transitions of Ce³⁺, Pr³⁺ and Tb³⁺ in the host lattices are assigned and corroborated. A convenient experiment formulation on the relationship between the lowest f-d transition energies and n value for trivalent 4fⁿ-series rare earth ions in these host lattices is applied.     

Thermal and photoluminescence properties of hydrated YPO4:Eu nanowires

In this work, we used the solution precipitation route to synthesize Eu³⁺-doped YPO₄·nH₂O nanowires. The structure, morphology, composition, thermal behavior, and photoluminescence of as-synthesized product were characterized by X-ray diffraction (XRD), thermogravimetric and differential thermal analysis (TG/DTA), energy-dispersive X-ray spectroscopy (EDS), Fourier transform infrared spectroscopy (FT-IR), field emission scanning electron microscopic (FE-SEM) and photoluminescence (PL) spectra. The dependence of the structure, morphology, composition and luminescent properties on the thermal treatment was investigated. The results indicate that the aqueous synthesis has a better control on the structure, morphology, composition of the products, and that the heat treatment induces the transitions of the structure, composition, and luminescent properties.     

Syntheses, crystal structures and spectroscopic properties of KEu[AsS4], K3Dy[AsS4]2 and Rb4Nd0.67[AsS4]2

Three rare earth compounds, KEu[AsS₄] (1), K₃Dy[AsS₄]₂ (2), and Rb₄Nd_0.67[AsS₄]₂ (3) have been synthesized employing the molten flux method. The reactions of A₂S₃ (A = K, Rb), Ln (Ln = Eu, Dy, Nd), As₂S₃, S were accomplished at 600 °C for 96 h in evacuated fused silica ampoules. Crystal data for these compounds are: 1, monoclinic, space group P2₁/m (no. 11), a = 6.7276(7) Å, b = 6.7190(5) Å, c = 8.6947(9) Å, β = 107.287(12)°, Z = 2; 2, monoclinic, space group C2/c (no. 15), a = 10.3381(7) Å, b = 18.7439(12) Å, c = 8.8185(6) Å, β = 117.060(7)°, Z = 4; 3, orthorhombic, space group Ibam (no. 72), a = 18.7333(15) Å, b = 9.1461(5) Å, c = 10.2060(6) Å, Z = 4. 1 is a two-dimensional structure with ²_∞[Eu(AsS₄)]⁻ layers separated by potassium cations. Within each layer, distorted bicapped trigonal [EuS₈] prisms are linked through distorted [AsS₄]³⁻ tetrahedra. Each Eu²⁺ cation is coordinated by two [AsS₄]³⁻ units by edge-sharing and bonded to further two [AsS₄]³⁻ units by corner-sharing. Compound 2 contains a one-dimensional structure with ¹_∞[Dy(AsS₄)₂]³⁻ chains separated by potassium cations. Within each chain, distorted bicapped trigonal prisms of [DyS₈] are linked by slightly distorted [AsS₄]³⁻ tetrahedra. Each Dy³⁺ ion is surrounded by four [AsS₄]³⁻ moieties in an edge-sharing fashion. For compound 3 also a one-dimensional structure with ¹_∞[Nd₀.₆₇(AsS₄)₂]⁴⁻ chains is observed. But the Nd position is only partially occupied and overall every third Nd atom is missing along the chain. This cuts the infinite chains into short dimers containing two bridging [As₄]³⁻ units and four terminal [AsS₄]³⁻ groups. 1 is characterized with UV/vis diffuse reflectance spectroscopy, IR, and Raman spectra.     

Sm2NiSn4: The intermediate structure type between ZrSi2 and CeNiSi2

A new rare earth nickel stannide, Sm₂NiSn₄, has been prepared by reacting the pure elements at high temperature in welded tantalum tubes. Its crystal structure was established by single crystal X-ray diffraction studies. Sm₂NiSn₄ crystallizes in the orthorhombic space group Pnma (No. 62) with cell parameters of a=16.878(2) Å, b=4.4490(7) Å, c=8.915(1) Å, and Z=4. Its structure can be viewed as the intermediate type between ZrSi₂ and CeNiSi₂. Sm₂NiSn₄ features two-dimensional (2D) corrugated [NiSn₄]⁶⁻ layers in which the 1D Sn zigzag chains and the 2D Sn square sheets are bridged by Ni atoms. The Sm³⁺ cations are located at the interlayer space. Results of both resistivity measurements and extended-Hückel tight-binding band structure calculations indicate that Sm₂NiSn₄ is metallic.     

Crystal structure and electrical properties of the mixed valent titanium oxysulfide Sm2Ti2S2O4.5

A new phase Sm₂Ti₂S₂O_4.5 was synthesized and its crystal structure was solved by single-crystal X-ray diffraction. This compound crystallizes in the monoclinic system (C2/m) with lattice constants a=17.9987(11) Å, b=3.71607(14) Å, c=12.6172(8) Å and β=133.645(4)°. The structure is built up from double chains of Ti-centered octahedra between which Sm-polyhedra develop. In spite of very close formulations, the structure of Sm₂Ti₂S₂O_4.5 differs completely from that of the defect Ruddelsden-Popper phase Sm₂Ti₂S₂O₅ previously reported. The title compound presents a mixed valence for titanium with Ti(III) (d¹) and Ti(IV) (d⁰) located in different crystallographic sites. However, conductivity measurements show that this compound is non-metallic.     

Ca5(PO4)3Cl中铕和铽间的电子转移

本文通过对铕和铽在Ca₅(PO₄)₃Cl基质中的发光特征的研究，发现铕和铽之间存在着电子转移现象，并对其反应机理进行了探讨。Eu³⁺(4f⁶)和Tb³⁺(4f⁸)通过电子转移使它们达到电子结构稳定的Eu²⁺(4f⁷)和Tb⁴⁺(4f<     

Tunable photoluminescence of NaYF4:Eu nanocrystals by Sr codoping

NaYF₄:Eu/Sr nanocrystals were synthesized by a hydrothermal method. Tunable photoluminescence of the NaYF₄:Eu nanocrystals was successfully achieved by codoping with Sr²⁺ ions. With increasing Sr²⁺ concentration, not only the X-ray diffraction peaks of the nanocrystals become broader, but also the positions of them shift toward larger lattice parameters. Eu³⁺ and Eu²⁺ have been found to coexist in an NaYF₄:Eu/Sr. The Eu³⁺/Eu²⁺ emission intensity ratio changed with the Sr²⁺ concentration and excitation wavelength. More interestingly, the spectral configurations of Eu²⁺ and Eu³⁺ also varied with the excitation wavelength, indicating that the nanocrystals have multiple luminescence centers or emitting states.