稀土离子与牛血Cu（Zn）—SOD的作用

采用ＥＳＲ、ＣＤ谱和荧光光谱研究了ｐＨ＝６．３时六次甲基四胺－ＨＣｌ缓冲溶液中ＬａＣｌ３和ＴｂＣｌ３与Ｃｕ（Ｚｎ）－ＳＯＤ的配位作用和结构。Ｃｕ（Ｚｎ）－ＳＯＤ可增强Ｔｂ＾３＋的荧光发射，Ｔｂ＾３＋与Ｃｕ（Ｚｎ）－ＳＯＤ有多个配位位置，其中有２个强结合位点，Ｌａ＾３＋可Ｔｂ＾３＋可竞争Ｃｕ（Ｚｎ）…ＳＯＤ上相同结合位点，７７Ｋ下Ｌａ＾３＋与Ｔｂ＾３＋使Ｃｕ（Ｚｎ）－ＳＯＤ的Ｃｕ＾２＋活性中心的配位     

铽离子荧光探针对酶与金属离子间能量转移和结合位的研究

应用荧光光度法研究了Ｔｂ＾３＋与牛胰脱氧核糖核酸酶（ＢＰＤ），枯草杆菌α－淀粉酶（ＢＳα－Ａ）的络合发光现象，实验表明，ＢＰＤ和ＢＳα－Ａ分别在ＰＨ＝７－８和５－６范围内与Ｔｂ＾３＋络合，并发射Ｔｂ＾３＋的特征荧光，Ｔｂ＾３＋与ＢＰＤ和ＢＳα－Ａ的络合比分别为２：１和４：１。并应用Ｆｏｒｓｔｅｒ理论测定了Ｔｂ＾３＋与ＢＰＤ和ＢＳα－Ａ之间能量传递的距离Ｒ分别为１．３９ｎｍ和１．４８ｎｍ，其临界距离     

吡嗪－2，3－二羧酸体系导数荧光法同时测定铕、铽

研究了以吡嗪－２，３－二羧酸（ＰＹＤＡ）为荧光试剂应用导数荧光技术同时测定Ｅｕ~（３＋）、Ｔｂ~（３＋）的最佳条件、共存离子的影响和Ｅｕ~（３＋）、Ｔｂ~（３＋）－ＰＹＤＡ配合物的配合比、稳定常数及发光机理。Ｅｕ~（３＋）、Ｔｂ~（３＋）的检测限分别达４．０和２．０ｎｇ／ｍＬ，利用本方法成功地测定了稀土试样中铕、铽的含量。     

植物细胞外钙调素的稀土发光探针研究

从植物中提纯了细胞外钙调素（ＣａＭ），并利用ＮＡＤ激酶激活作用及拮抗剂的抑制作用进行了ＣａＭ特性试验。利用稀土（Ｔｂ＾３＋）发光探针测得胞外ＣａＭ具有４个金属离子结合位点。敏化Ｔｂ＾３＋激发光谱结果证明其含有１个Ｔｙｒ残基。胞外ＣａＭ（Ｙｙｒ?能够向Ｔｂ３＋传能并使Ｔｂ３＋特征发光增强。根据Ｆｏｒｓｔｅｒ能量传递理论测得胞外ＣａＭ中Ｔｙｒ→Ⅲ，Ⅳ位之间距离分别为１．１０４和１．０５６ｎｍ，它们均小     

Gd_xY_（1－x）P_5O_（14）：Ce，Tb的发光和能量传递Ⅱ．Ce→

研究了Ｇｄ＿ｘＹ＿（１－ｘ）Ｐ＿５Ｏ＿（１４）：Ｃｅ＿（０．０１），Ｔｂ＿（０．０２）体系中Ｇｄ的子晶格在Ｃｅ→Ｇｄ→Ｔｂ能量传递中的中介作用规律及ＧｄＰ＿５Ｏ＿（１４），ＧｄＰ＿５Ｏ＿（１４）：Ｃｅ，ＧｄＰ＿５Ｏ＿（１４）：Ｔｂ和Ｇｄ＿ｘＹ＿（１－ｘ）Ｐ＿５Ｏ＿（１４）：Ｃｅ，Ｔｂ的荧光光谱、激发光谱。结果表明，当ｘ＞０．７时，结构从单斜Ⅱ（Ｃ２／ｃ）的层状结构变为单斜Ｉ（Ｐ２＿１／ｃ）的带状结构，Ｃｅ￣（３＋）的发射光谱和Ｇｄ￣（３＋）的吸收光谱交迭增加等是Ｃｅ￣（３＋）→Ｇｄ￣（３＋）→Ｔｂ￣（３＋）能量传递几率增加的主要原因。     

铽—镧（镥,钇）—均苯四甲酸共发荧光体系的研究和应用

研究发现Ｌａ＾３＋（Ｌｕ＾３＋，Ｙ＾３＋）对Ｔｂ＾３＋均苯四甲酸（ＢＴＣＡ）体系具有强烈的共发荧光效应，在最佳条件下，共发光离子Ｌａ＾３＋，Ｌｕ＾３＋，Ｙ＾３＋可分别使Ｔｂ－ＢＴＣＡ体系的荧光增强３１２，１３３和１００倍，介绍了Ｔｂ－Ｌａ（Ｌｕ，Ｙ）－ＢＴＣＡ共发荧光体系的荧光特点，形成条件和影响因素，利用Ｌａ＾３＋（Ｌｕ＾３＋，Ｙ＾３＋）的增敏效应，测定了合成稀土样品和包头稀土标准氧化物中的Ｔｂ     

烯土—铌（钽）复合溴氧化物的结构与光谱特性

用高温固相法合成了系列化合物ＲＥ０．０６Ｌａ０．９４Ｍ２Ｏ６Ｂｒ（Ｍ＝Ｎｂ，Ｔａ；ＲＥ＝Ｅｕ，Ｔｂ，Ｐｒ，Ｓｍ），并测定了其激发和发射光谱。室温下Ｅｕ＾３＋，Ｔｂ＾３＋，Ｐｒ＾３＋，Ｓｍ＾３＋在稀土－铌（钽）复合溴氧化物中呈现特征激发谱线，但Ｎｂ和Ｔａ的光谱特性稍有不同。     

水杨酸酯—Triton X—100—镥（Ⅲ）（钆（Ⅲ））增敏体系荧光法测定铽和镝

１引言作者等曾报道水杨酸苯酯－ＴｒｉｔｏｎＸ－１００－Ｇｄ３＋增敏体系荧光法测定Ｔｂ３＋。为了进一步提高测定的灵敏度并探讨同时测定Ｄｙ３＋的可能性，本文探讨了乙、丁、戊酯等烷基酯对测定的影响。结果表明，丁酯体系的灵敏皮最高，在该体系中Ｄｙ３＋的特征荧光也明显加强，在Ｌｕ３＋共存下Ｔｂ３＋、Ｄｙ３＋的检测限分别达到０．２和８．０μｇ／Ｌ，对Ｔｂ３＋而言，灵敏度较苯酯－Ｇｄ３＋增敏体系提高了１０倍。２实验部分２．１试剂与仪器１ｇ／ＬＴｂ３＋、Ｄｙ３＋标准溶液；３．５×１０－２ｍｏｌ／Ｌ水杨酸酯（乙、…     

稀土发光配合物的研究Ⅱ.稀土,3-吡啶甲酸,邻菲咯啉三元配合物的合成和荧光性质

合成了１４种稀土元素与３吡啶甲酸（ＨＬ）及邻菲咯啉（Ｐｈｅｎ）的三元配合物,通过元素分析和化学分析确定其化学组成为ＲＥＬ３·Ｐｈｅｎ,并利用ＩＲ、ＵＶ、１ＨＮＭＲ、ＴＧＤＴＡ和Ｘ射线粉末衍射等手段对配合物进行了表征．研究了Ｅｕ（Ⅲ）及Ｔｂ（Ⅲ）配合物的荧光性质．     

GdxY1—XP5O14：Ce,Tb的发光和能量传递：Ⅰ.制备,结构和光谱性质

研究了稀土五磷酸盐Ｇｄｘ１－ＸＰ５Ｏ１４：Ｃｅ，Ｔｂ体系的制备，结构和光谱性质。当ｘ＞０．７时，该材料属单斜晶系Ｉ，Ｐ２１／ｃ结构，当≤０．７时，属单斜晶系Ⅱ，Ｃ２／ｃ结构。研究了ＧｄＰ５Ｏ１４：Ｃｅ，Ｔｂ６ ＹＰ５Ｏ１４：Ｃｅ，Ｔｂ的荧光光谱，确定了通过基质Ｇｄ离子中介的Ｃｅ＾３＋→Ｇｄ＾３＋→Ｔｂ＾３＋能量传递的现象。     

Controllable synthesis and luminescent properties of three-dimensional nanostructured CaWO4:Tb3+ microspheres

Three-dimensional (3D) nanostructured CaWO(4):Tb(3+)microspheres assembled by submicrospindles were synthesized via a mild sonochemical route from an aqueous solution of CaCl(2), TbCl(3) and Na(2)WO(4) with the aid of surfactant Polyglycol 600 (PEG-600). The crystal structure and morphology of the as-prepared products were characterized by using X-ray diffraction (XRD) and field emission scanning electron microscopy (FE-SEM). Rietveld refinement was carried out on the XRD data. The results showed that the CaWO(4):Tb(3+)nanoparticles can be formed without ultrasonic irradiation or addition of PEG-600. With continuously increasing irradiation time the submicrospindles and microspheres could be self-assembled. The central diameter and length of the submicrospindles are around 190 and 500 nm, respectively. The 3D CaWO(4):Tb(3+)nanostructured microspheres with diameter of 2-4 μm were assembled by the submicrospindles. A possible formation mechanism for the 3D-structured CaWO(4):Tb(3+)microspheres was proposed. The Photoluminescent (PL) properties of Tb(3+) ions in the nanostructured CaWO(4) microspheres were studied. The energy transfer processes in CaWO(4):Tb(3+)microspheres were analyzed. The electric dipole-dipole energy transfers related to (5)D(3) level were studied by inspecting the fluorescence decay of (5)D(3) level. The energy transfer critical distance was estimated.     

The quantum cutting of Tb(3+) in Ca(6)Ln(2)Na(2)(PO(4))(6)F(2) (Ln = Gd, La) under VUV-UV excitation: with and without Gd(3+)

The VUV-vis spectroscopic properties of Tb(3+) activated fluoro-apatite phosphors Ca(6)Ln(2-x)Tb(x)Na(2)(PO(4))(6)F(2) (Ln = Gd, La) were studied. The results show that phosphors Ca(6)Gd(2-x)Tb(x)Na(2)(PO(4))(6)F(2) with Gd(3+) ions as sensitizers have intense absorption in the VUV range. The emission color of both phosphors can be tuned from blue to green by changing the doping concentration of Tb(3+) under 172 nm excitation. The visible quantum cutting (QC) via cross relaxation between Tb(3+) ions was observed in cases with and without Gd(3+). Though QC can be realized in phosphors Ca(6)La(2-x)Tb(x)Na(2)(PO(4))(6)F(2), we found that Gd(3+)-containg phosphors have a higher QC efficiency, confirming that the Gd(3+) ion indeed plays an important role during the quantum cutting process. In addition, the energy transfer process from Gd(3+) to Tb(3+) as well as (5)D(3)-(5)D(4) cross relaxation was investigated and discussed in terms of luminescence spectra and decay curves.     

K3[Tb(x)Eu(1-x)Ge3O8(OH)2] (x = 1, 0.88, 0.67, 0): 2D-layered lanthanide germanates with tunable photoluminescent properties

A family of novel 2D-layered lanthanide germanates K(3)[Tb(x)Eu(1-x)Ge(3)O(8)(OH)(2)] (x = 1, 0.88, 0.67, 0; denoted as TbGeO-JU-87, Tb(0.88)Eu(0.12)GeO-JU-87, Tb(0.67)Eu(0.33)GeO-JU-87, and EuGeO-JU-87) were synthesized under mild hydrothermal conditions in a concentrated gel system. They are isostructural, as confirmed by the powder X-ray diffraction analysis. The single-crystal X-ray diffraction analysis of EuGeO-JU-87 reveals that it is a 2D-layered [EuGe(3)O(8)(OH)(2)](n)(3n-) anionic framework, which is built up from GeO(4)H/GeO(4) tetrahedra and EuO(6) octahedra by sharing vertex O atoms. Charge neutrality is achieved by K(+) ions located in the free void space. Interestingly, photoluminescence studies show that Tb(0.88)Eu(0.12)GeO-JU-87 and Tb(0.67)Eu(0.33)GeO-JU-87 exhibit a high Tb(3+)-to-Eu(3+) energy-transfer efficiency and the Tb(x)Eu(1-x)GeO-JU-87 system displays tunable photoluminescent properties.     

Lightly doping Ca2+ in perovskite PrCoO3 for tailored spin states and electrical properties

A series of Pr(1-x)Ca(x)CoO(3) samples were prepared using a novel molten salt reaction that is convenient to obtain single phases avoiding aggregates compared to conventional solid state reactions. The formation reaction was monitored by X-ray diffraction combined with thermal analysis, and all samples were characterized by X-ray diffraction, scanning electron microscopy, Fourier transform infrared spectroscopy, and alternating current impedance. It is demonstrated that all Pr(1-x)Ca(x)CoO(3) samples crystallized in a pure orthorhombic perovskite structure. By increasing the doping level, the symmetry of the orthorhombic structure was enhanced, and is followed by an increase in the population of Co(3+) in the intermediate spin state. All samples exhibited typical semiconducting behavior, showing conductivities highly dependent on the Ca(2+) doping. The conduction for x = 0 shows a simple thermal activated process, which changed into a Mott's variable range hopping mechanism for x > 0. By increasing the Ca(2+) doping level, the relevant activation energy is decreased, while the density of the localized electronic state is increased.     

The behavior of mixed-metal oxides: physical and chemical properties of bulk Ce1-xTbxO2 and nanoparticles of Ce1-xTbxOy

The physical and chemical properties of bulk Ce(1-x)Tb(x)O(2) and Ce(1-x)Tb(x)O(y) nanoparticles (xTb exchange nor the introduction of oxygen vacancies in Ce(1-x)Tb(x)O(y) significantly affect the charge on the Ce cations. In contrast, the O K-edge and Tb L(III)-edge XANES spectra for Ce(1-x)Tb(x)O(y) nanoparticles show substantial changes with respect to the corresponding spectra of Ce and Tb single oxide references. The Ce(0.5)Tb(0.5)O(y) compounds exhibit a much larger Tb(3+)/Tb(4+) ratio than TbO(1.7). A comparison with the properties of Ce(1-x)Zr(x)O(y) and Ce(1-x)Ca(x)O(y) shows important differences in the charge distribution, the magnitude of the dopant induced strain in the oxide lattice, and a superior behavior in the case of the Ce(1-x)Tb(x)O(y) systems. The Tb-containing oxides combine stability at high temperature against phase segregation and a reasonable concentration of O vacancies, making them attractive for chemical and catalytic applications.     

Patterning of Gd2(WO4)3:Ln3+ (Ln=Eu, Tb) luminescent films by microcontact printing route

Gd(2)(WO(4))(3) doped with Eu(3+) or Tb(3+) thin phosphor films with dot patterns have been prepared by a combinational method of sol-gel process and microcontact printing. This process utilizes a PDMS elastomeric mold as the stamp to create heterogeneous pattern on quartz substrates firstly and then combined with a Pechini-type sol-gel process to selectively deposit the luminescent phosphors on hydrophilic regions, in which a Gd(2)(WO(4))(3):Ln(3+) (Ln=Eu, Tb) precursor solutions were employed as ink. X-ray diffraction (XRD), scanning electron microscopy (SEM), photoluminescence (PL) spectra, as well as low voltage cathodoluminescence (CL) spectra were carried out to characterize the obtained samples. Under ultraviolet excitation and low-voltage electron beams excitation, the Gd(2)(WO(4))(3):Eu(3+) samples exhibit a strong red emission arising from Eu(3+)(5)D(0,1,2)-(7)F(1,2) transitions, while the Gd(2)(WO(4))(3):Tb(3+) samples show the green emission coming from the characteristic emission of Tb(3+) corresponding to (5)D(4)-(7)F(6,5,4,3) transitions. The results show that the patterning of rare earth-doped phosphors through combining microcontact printing with a Pechini-type sol-gel route has potential for field emission displays (FEDs) applications.     

Controlled fabrication and shape-dependent luminescence properties of hexagonal NaCeF4, NaCeF4:Tb3+ nanorods via polyol-mediated solvothermal route

Hexagonal monodisperse NaCeF(4) and NaCeF(4):Tb(3+) nanorods have been successfully synthesized by a polyol-mediated solvothermal route with ethylene glycol (EG) as solvent. The crystalline phase, size, morphology, and luminescence properties were characterized using X-ray diffraction (XRD), scanning electron microscopy (SEM), transmission electron microscopy (TEM), and photoluminescence (PL) spectra as well as dynamic decays. The experimental results indicate that the content of NH(4)F and NaNO(3) are crucial in controlling product morphology and size. Nanorods with different aspect ratios could be controllably obtained under settled conditions. Shape-dependent luminescence and energy transfer routes from Ce(3+) to Tb(3+) in NaCeF(4):Tb(3+) nanorods were observed by the modified local crystal field environment around rare earth ions. The 4f-5d transitions of Ce(3+) ions have much higher sensitivity to the anisotropic shape of samples than that of Tb(3+) ions.     

Structure Refinement and Two-Center Luminescence of Ca(3)La(3)(BO(3))(5):Ce(3+) under VUV-UV Excitation

A series of Ca(3)La(3(1-x))Ce(3x)(BO(3))(5) phosphors were prepared by a high-temperature solid-state reaction technique. Rietveld refinement was performed using the powder X-ray diffraction (XRD) data, which shows occupation of Ce(3+) on both Ca(2+) and La(3+) sites with a preferred location on the La(3+) site over the Ca(2+) site. The prepared samples contain minor second phase LaBO(3) with contents of ～0.64-3.27 wt % from the Rietveld analysis. LaBO(3):1%Ce(3+) was prepared as a single phase material and its excitation and emission bands were determined for identifying the influence of impurity LaBO(3):Ce(3+) luminescence on the spectra of the Ca(3)La(3(1-x))Ce(3x)(BO(3))(5) samples. The luminescence properties of Ca(3)La(3(1-x))Ce(3x)(BO(3))(5) samples under vacuum ultraviolet (VUV) and UV excitation were investigated, which exhibited two-center luminescence of Ce(3+), assigned to the Ce(1)(3+) center in the La(3+) site and Ce(2)(3+) center in the Ca(2+) site, taking into account the spectroscopic properties and the Rietveld refinement results. The influences of the doping concentration and the excitation wavelength on the luminescence of Ce(3+) in Ca(3)La(3(1-x))Ce(3x)(BO(3))(5) are discussed together with the decay characteristics.     

Unusual Luminescence of Ca8[Al12O24]（WO4）2： Tb^3＋

The luminescence properties of aluminate sodalite Ca8[Al12024](WO4)2 (CAW) undoped and doped with Th^3 are reported and discussed. At room temperature the emission of tetrahedral WO4^2- in CAW showed an abnormally small Stokes shift (9060 cm^-1), which is related to the crystal structure of CAW. A strong absorption band in the excitation spectrum of the Th^3 -activated CAW is ascribed to the absorption of the charge transfer state Th^4 -W^5 , into which the excitation resulted in the efficient emission from the ^5D4 level of Tb^3 , but not from the ^5D3 level.     

Synthesis and Characterization of Highly Efficient Photoluminescence Gd doping Hexagonal CePO_4 (One-dimensional Nanowires)

Rare earth phosphates have been used extensively in luminescent phosphors. Hexagonal Ce_(1-x)Gd_xPO_4 with crystal field manipulation was successfully synthesized using a hydrothermal method. The photoluminescence emission intensity of hexagonal CePO_4 was obviously enhanced by the crystal structure manipulation with gadolinium ions codoping. Compared to pure CePO_4, the intensity photoluminescence was enhanced about 15 folds with x = 0.05. The effect of gadolinium doping was systematically investigated by X-ray diffraction, transmission electron microscopy, X-ray photoelectron spectroscopy and photoluminescence spectroscopy. Crystal field asymmetry can be effectively tuned by different amount of Gd~(3+) codoping, and the crystal field asymmetry is conductive to electron population of high energy level of Ce~(3+) ions. This material has potential applications in optics, electronics fields, and so on. Meanwhile, the method can be extended to another kind of high performance photoluminescence materials preparation.