Ca1-xZnxTiO3:Pr3+的固溶特性及其发光性能

通过高温固相合成法制备了名义组成为Ca1-xZnxTiO3：Pr^3＋（x=0．0～0．20）的红色发光材料，采用XRD和光谱等手段研究微量Zn掺杂的单相Ca1-xZnxTiO3：Pr^3＋材料的晶体结构参数与发光性能，分析了等价Zn^2＋的掺杂对固溶体结构参数与发光性能的影响规律。结果表明，在x≤0．01微量Zn掺杂时，Zn取代Ca形成单相Ca1-xZnxTiO3：Pr^3＋固溶；其晶胞参数和晶胞体积，260和330nm两激发带以及610nm发射峰强度均随Zn掺量增加快速减小，且发光强度与晶胞参数的变化规律相吻合。分析表明这种变化与Zn取代Ca形成的固溶结构有关。     

Ca_(1-x)Zn_xTiO_3∶Pr~(3 ),R~ (R~ =Li~ ,Na~ ,K~ ,Rb~ ,Cs~ ,Ag~ )的合成和发光性质

采用X射线衍射、荧光光谱和热释发光研究了Ca1 -xZnxTiO3∶Pr3 ,R 的物相组成和发光性质。Pr3 取代Ca2 形成PrCa·正电性缺陷发光中心。激发光谱是峰值位于 3 3 0nm附近的宽带谱 ,发射光谱是峰值在 613nm半宽度为 2 0nm的带谱 ,对应Pr3 的1 D2 -3H4 跃迁发射。发光强度和余辉随基质组分Zn/Ca摩尔比和合成温度而变化。Zn2 的最佳含量在 10 %～ 2 0 %。X射线衍射研究表明掺入适量的Zn2 物相组成为CaTiO3,Ca2 Zn4 Ti1 5O36 和Zn2 TiO4 。热释发光曲线表明掺入Zn2 离子后体系中形成了新的缺陷ZnTi″ ,且ZnTi″的缺陷陷阱深度大于RCa′。     

微乳液法制备MAl2O4：Eu^2＋，Dy^3＋（M=Ca，Sr，Ba）发光材料及其发光性能

采用微乳液法合成了MAl2O4：Eu^2＋，Dy^3＋（M=Ca，Sr，Ba）长余辉发光材料，并对其晶体结构和发光性能进行了比较与讨论。XRD分析表明，所合成的Ca2O4：Eu^2＋，Dy^3＋，SrAl2O4：Eu^2＋，Dy^3＋粉体为单斜晶系结构，BaAl2O4：Eu^2＋，Dy^3＋粉体为六方晶体结构。MAl2O4：Eu^2＋，Dy^3＋（M=Ca，Sr，Ba）发光材料的激发光谱都为一宽带连续谱，表明从紫外至可见光均可有效的激发该材料。发射光谱的发射波长峰值分别为440nm（M=Ca），520nm（M=Sr）和496nm（M=Ba）。对应的发光颜色分别为蓝色、黄绿色和蓝紫色。余辉衰减曲线分为快衰减、中间过渡衰减和随后极长的慢衰减过程，符合双曲线方程I=At^-n，余辉亮度与时间顺序为Sr〉Ca〉Ba。     

R3GeVO9（R=Y，La）：Eu^3＋（或Dy^3＋）的合成及其发光性质

采用高温固相法台成了稀土复合钒锗酸盐R3GeVO9(R=Y,La)体系，并以此为基质研究了Eu^3 和Dy^3 在其中的发光性质，以Eu^3 为结构探针探讨了En^3 在R3GeVO9(R=Y,La)中的格位情况。同时，还研究了被取代离子R^3 Z／r对Eu^3 的红橙比和Dy^3 的黄蓝比的影响以及浓度、温度和Bi^3 对它们发光强度的影响。     

利用热释光和光激励技术研究合成工艺对BaFBr：Eu^2＋,Al^3＋发光性质的影响

利用热释发光谱和光激励发光谱表征了不同合成工艺条件对合成BaFBr:Eu^2 ,Al^3 发光性质的影响，利用理论分析找出了热释发光衰减与光激励衰减的异同，理论上计算了不同的合成工艺对BaFBr:Eu^2 ,Al^3 色心能级的影响，其热释发光谱和光激励发光谱的理论计算值能较好的吻合，并且能够很好的表征实验结果。     

杂质的添加对SrAl2O：Eu^2＋,Dy^3＋余辉发光特性的改善

采用溶胶－凝胶法制备SrAl2O4:Eu^2 ,Dy^3 磷光体,并在合成过程中添加硼或硅以探讨光致发光及长余辉发光性质。发现硼、硅添加物不仅是助熔剂,且能改良SrAl2O4:Eu^2 ,Dy^3 之长余辉的持续时间及余辉发光强度。基于不同磷光体样品的实验结果比较,综合材料表面微结构观察、X射线衍射图谱、热释发光光谱与余辉衰减曲线的测量等实验结果分析,推断在SrAl2O4:Eu^2 ,Dy^3 中添加硼、硅可导致磷光体缺陷增加并稳定活化剂Eu^2 的价态。     

红色长余辉发光材料Ca2Zn4Ti15O36：Pr^3＋的合成和发光性质

分别采用高温固相法和溶胶-凝胶法合成了新型红色长余辉发光材料Ca2Zn4Ti15O36:Pr。高温固相法合成Ca2Zn4Ti15O36需要在1200℃灼96h才能形成纯物相。热重分析曲线和X射线衍射分析结果表明：溶胶-凝胶法制得的前驱体在700℃灼烧12h开始形成Ca2Zn4Ti15O36物相；在1000℃灼烧24h得到Ca2ZnTi15O36纯物相；最佳反应温度为1000℃，激活剂Pr^3 的最佳浓度为0．6mol％，发光强度比高温固相法增强了510％。     

用3种方法合成Y3Al5O12：RE^3＋（RE=Eu,Dy）发光粉的对比研究

以金属硝酸盐为反应原料,分别采用柠檬酸－凝胶法、共沉淀法和固相法制备了YAG和YAG：RE^3 (RE=Eu,Dy)（1％,摩尔分数）发光粉,并通过XRD,TG－DTA和发光光谱对样品进行了表征。柠檬酸－凝胶法、共沉淀法和固相法制备的YAG和YAG：Eu的晶相形成温度分别是800和900℃。Eu^3 在非晶态和晶态YAG中其激发和发射光谱有明显差异,在一定温度范围内,发光强度随烧结温度的升高而增强。由于碳杂质的存在,900和1000℃下柠檬酸－凝胶法制备样品的发射强度较其他两种方法低。     

溶胶—凝胶合成（Mg,Ca）O—SiO2：Eu^3＋,Bi^3＋发光体及其发光行为

以Ｍｇ（ＮＯ３）２，Ｃａ（ＮＯ３）２，Ｅｕ（ＮＯ３）３，Ｂｉ（ＮＯ３）３和Ｓｉ（ＯＣ２Ｈ５）４为反应物，采用溶胶－凝胶法，在比较低的温度，首次合成０．７０１ｍｏｌＭｇＯ－０．１７５ｍｏｌＣａＯ－１．２５ｍｏｌＳｉＯ２：０．０６ｍｏｌＥｕ＾３＋，０．００２ｍｏｌＢｉ＾３＋（加入Ｌｉ＾＋作为电荷补偿剂）发光体，得到了最佳合成条件，研究了由溶胶向凝胶转变和凝胶向发光晶体的转变过程，探讨了发光体在不同激光     

（ZnBaLa）BO3：Eu^3＋的合成与发光的研究

高温固相扩散法合成了发光材料Zn1．5xBa1．5yLa1-x-y-z)BO3∶Eu3+z(x+y+z＜0．4)．对样品进行了XRD和IR分析,结果表明：在空气中900 ℃条件下,合成了荧光体样品,LaBO3中La3+离子被部分Zn2+和Ba2+离子取代使晶系发生了变化,LaBO3属于正交晶系,而(Zn0．27Ba0．24La0．61)BO3∶Eu3+0．05经过XRD属于立方晶系,a=0.639 7,V=0.261 8 nm3．扫描电镜测其晶貌,平均粒度为22 μm左右．样品的激发光谱和发射光谱显示：在基质BO3结构中O2—Eu3+的CT带位于295 nm,Eu3+的强发射来自5D0→7F1和5D0→7F2跃迁,存在磁偶极和电偶极两种跃迁．     

Electron spectroscopic investigation of metal-insulator transition in Ce1-xSrxTiO3

We have carried out detailed electron spectroscopic investigation of Ce_1−x Sr_xTiO₃ exhibiting insulator-metal transition withx. Core level X-ray photoelectron spectra of Ce3d as well as resonant photoemission spectra obtained at the Ce4d→4f resonant absorption threshold establish Ce as being in the trivalent state throughout the series. Using the ’off-resonance’ condition for Ce 4f states, we obtain the Ti3d dominated spectral features close toE _F , exhibiting clear signatures of coherent and incoherent peaks. We discuss the implications of our findings in relation to the metalinsulator transition observed in this series of compounds. Dedicated to Professor C N R Rao on his 70th birthday     

Ca0.61Nd0.26TiO3粉体：熔盐法制备及烧结特性

钙钛矿结构的(Ca1-xLn2/3x)TiO3体系是CaTiO3中的Ca2+被三价的稀土离子Ln3+(hn,Nd和Sm等稀土元素)不等价置换所形成的固溶体,该固溶体具有高介电常数、高品质因数等特点[1,2],这在微波器件小型化应用中具有重要的意义.     

Ca9Y(PO4)7:Ce3+,Tb3+纳米荧光粉的制备及发光性能

采用水热法制备出Ca₉Y（PO₄）₇：Ce³⁺,Tb³⁺纳米荧光粉,通过XRD、SEM和荧光光谱等对样品进行了分析,研究在Ca₉Y（PO₄）₇基质中引入Ce³⁺,Tb³⁺离子对发光性能的影响规律。研究发现因Tb³⁺离子自身能量交叉驰豫的存在,使得单掺Tb³⁺时,通过调节Tb³⁺离子的浓度可以实现对发光颜色的控制。同时研究了Ce³⁺-Tb³⁺之间的能量传递为电多极相互作用的偶极-四极机制,Ce³⁺-Tb³⁺之间最大的能量传递效率为55.6%。Ca₉Y（PO₄）₇：Ce³⁺,Tb³⁺的发光颜色可以通过激活离子之间的能量传递和共发射得到可控调节。SEM分析表明荧光粉颗粒尺寸在100 nm左右,分散性好。     

Magnetic properties of Ca2F2-xMnxO5

Magnetic susceptibility of Ca₂F_2-xMn_xO₅ members crystallizing in two different structures, one having octahedral (O), tetrahedral (T) and square-pyramidal (SP) coordination of transition metal atoms (OTSP structure) and the other having octahedral and tetrahedral coordination (OT structure), has been investigated. Susceptibility behaviour of the oxides with OTSP structure is different from that of the oxides with OT structure. Ca₂Fe_1-33Mn_0-67O₅ with OTSP structure shows an antiferromagnetic ordering while the corresponding oxide with OT structure shows weak ferromagnetism. Contribution No. 398 from the Solid State and Structural Chemistry Unit     

Crystal growth, structural characterization and magnetic properties of Ca3CuRhO6, Ca3Co1.34Rh0.66O6 and Ca3FeRhO6

Single crystals of Ca₃CuRhO₆, Ca₃Co_1.34Rh_0.66O₆ and Ca₃FeRhO₆ were synthesized by high temperature flux growth in molten K₂CO₃ and structurally characterized by single crystal X-ray diffraction. While Ca₃Co_1.34Rh_0.66O₆ and Ca₃FeRhO₆ crystallize with trigonal (rhombohedral) symmetry in the space group , Z=6: Ca₃Co_1.34Rh_0.66O₆a=9.161(1) Å, c=10.601(2) Å; Ca₃FeRhO₆a=9.1884(3) Å, c=10.7750(4) Å; Ca₃CuRhO₆ adopts a monoclinic distortion of the K₄CdCl₆ structure in the space group C2/c, Z=4: a=9.004(2) Å, b=9.218(2) Å, c=6.453(1) Å, β=91.672(5). All crystals of Ca₃CuRhO₆ examined were twinned by pseudo-merohedry. Ca₃CuRhO₆, Ca₃Co_1.34Rh_0.66O₆, and Ca₃FeRhO₆ are structurally related and contain infinite one-dimensional chains of alternating face-sharing RhO₆ octahedra and MO₆ trigonal prisms. In the monoclinic modification, the copper atoms are displaced from the center of the trigonal prism toward one of the rectangular faces adopting a pseudo-square planar configuration. The magnetic properties of Ca₃CuRhO₆, Ca₃Co_1.34Rh_0.66O₆, and Ca₃FeRhO₆ are discussed.     

Structural,Magnetic and Optical Properties of BiFe1-xNbxO3

Nb doped multiferroic BiFe_1-xNb_xO₃ (0 <x <0.05) polycrystalline powders have been syn-thesized by using a sol-gel method. The effect of Nb dopant on the structural, magnetic and optical properties is investigated. According to the X-ray di raction data and the result of Rietveld re nement, all the samples maintain the R3c phase, while the lattice parameters a, c, the cell volume V and the Fe-O-Fe bond angle change. The remnant magnetization enhances by appropriate Nb doping due to the decreasing of the grain size. Meanwhile, Nb dopant leads to the narrowing of the band gap of BiFe_1-xNb_xO₃ samples.     

LaMnxFe1-xO3催化剂的制备及其对甲烷燃烧的催化性能

采用共沉淀法,以（NH₄）₂CO₃为沉淀剂制备钙钛矿型催化剂LaMn_xFe_1-xO₃（x=0, 0.2, 0.4, 0.6, 0.8, 1.0）,其结构和性能经XRD、 BET、 H₂-TPR、 SEM和TG-DSC表征。以催化甲烷燃烧为目标反应,考察了其催化性能,研究不同量离子掺杂对催化剂性能影响。结果表明：随着Mn离子掺杂量增加,催化剂的比表面积先变大后变小;LaMn_0.2Fe_0.8O₃的比表面积为42.1 m²·g^-1,催化活性最好,起燃温度T_l0%为400 ℃,完全转化温度T_90%为550 ℃。     

Structural and Magnetic Properties of Bi(Fe1-xMnx)O3

Bi(Fe_1-xMnx)O₃ bulk ceramics with Mn concentration x up to 0.3 were prepared by rapid sintering using sol-gel derived fine powders. Structure transformation is found to depend on the Mn doping concentration by X-ray diffraction and Raman spectroscopy. Bi(Fe_1-xMnx)O₃ maintains the rhombohedral structure of BiFeO3 with x=0.05 and 0.1, but changes to the orthorhombic structure with x=0.3. Weak ferromagnetism is observed for Bi(Fe_1-xMnx)O₃ with x=0.05 and 0.1, but stronger paramagnetism is observed for Bi(Fe_1-xMnx)O₃ with x=0.3 indicating a magnetic phase change from antiferromagnetic to paramagnetic with the structure changing from R3c to C222. Two anomalies at 30 and 140 K are observed for Bi(Fe_1-xMnx)O₃ with x=0.05 and 0.1. The anomaly at 30 K is concluded to be related to the freezing of cluster spin glass from dc magnetic memory and relaxation measurements.     

Ca9Y(PO4)7:Ce3+,Tb3+纳米荧光粉的制备及发光性能

采用水热法制备出Ca_9Y(PO4)7∶Ce~(3+),Tb~(3+)纳米荧光粉,通过XRD、SEM和荧光光谱等对样品进行了分析,研究在Ca_9Y(PO4)7基质中引入Ce~(3+),Tb~(3+)离子对发光性能的影响规律。研究发现因Tb~(3+)离子自身能量交叉驰豫的存在,使得单掺Tb~(3+)时,通过调节Tb~(3+)离子的浓度可以实现对发光颜色的控制。同时研究了Ce~(3+)-Tb~(3+)之间的能量传递为电多极相互作用的偶极-四极机制,Ce~(3+)-Tb~(3+)之间最大的能量传递效率为55.6%。Ca_9Y(PO4)7∶Ce~(3+),Tb~(3+)的发光颜色可以通过激活离子之间的能量传递和共发射得到可控调节。SEM分析表明荧光粉颗粒尺寸在100 nm左右,分散性好。     

Synthesis, Crystal Structure, and Magnetic Properties of Quasi-One-Dimensional Oxides Ca3CuMnO6 and Ca3Co1+xMn1−xO6

Synthesis conditions, crystal structures, and magnetic properties of quasi-one-dimensional complex oxides Ca₃CuMnO₆ (space group P-1, z=4, triclinic cell) and Ca₃Co_1+xMn_1−xO₆ with x=0, 0.25, 1.0 (structural type K₄CdCl₆, space group R-3c, z=6) are presented. The crystal structures of Ca₃CoMnO₆ and Ca₃CuMnO₆ were refined using neutron and combined X-ray and neutron diffraction analysis, respectively. The interatomic distances in oxygen polyhedra were found. In contrast to ferromagnetic Ca₃Co₂O₆ (T_c=24 K), manganese-containing phases Ca₃Co_1+xMn_1−xO₆ are characterized by antiferromagnetic interactions with Neel temperatures 18 K (x=0.25) and 13 K (x=0). For Ca₃CuMnO₆T_N was established to be 6 K.