一种基于形成杂多核络合物的荧光增敏效应的研究 Ⅲ.锰(Ⅱ)、钴(Ⅱ)的混合荧光增敏及其连续测定

本文研究了Mn~(2+)和Co~(2+)对7-(8-羟基-3,6-二磺基萘偶氮)-8-羟基喹啉-5-磺酸-硼砂反应体系的混合荧光增敏作用。实验条件下,荧光增敏强度满足线性加和关系的范围是:Mn~(2+)浓度0～2.9×10~(-7)mol/L;Co~(2+)浓度0～8.8×10~(-7)mol/L;总浓度不超过1.0×10~(-6)mol/L。检出限量为Mn~(2+)4.5×10~(-9)mol/L和Co~(2+)1.4×10~(-8)mol/L。实现了Mn~(2+)和Co~(2+)的连续测定。     

Triton X-100增敏桑色素荧光法测定痕量三苯基锡

pH4～5的介质中，三苯基锡（TPhT）与过量的桑色素（Morin）迅速形成络合物，此络合物能发较强的荧光，在适量的TritonX－100存在下，由于TritonX－100的增敏作用荧光大大增强。λex／λem＝415／525nm，三苯基锡在0．05×10－6～1．4×10－6mol／L范围内与荧光强度呈良好的线性关系，检出限1．2×10－9mol／L，用于实际水样测定，结果令人满意。     

胶束增敏荧光光度法测定土霉素的研究

提出了表面活性剂增敏的酸性降解荧光法测定土霉素的新方法。土霉素与浓H2SO4反应,生成强荧光降解物一脱水土霉素,在pH10.0的NH3 NH4Cl缓冲溶液中,CTMAB的存在对脱水土霉素的荧光有较强的增敏和增稳作用,土霉素含量在1.21×10-8mol/L～4.83×10-6mol/L范围内与荧光强度成正比,方法的检出限为6 66×10-9mol/L。应用本法测定片剂中的土霉素,平均回收率为99.6%(n=5)。     

尼尔雌醇的荧光光谱法研究与应用

系统研究了用荧光光谱法测定尼尔雌醇的条件。发现在中性条件下,β-CD能显著增敏荧光,探讨了作用机理,提出了测定尼尔雌醇的高灵敏度荧光光谱分析新方法。体系的线性范围为2.63×10-7~1.84×10-5mol/L,检出限为9.4×10-8mol/L。已用于市售尼尔雌醇片剂样品的分析。     

基于荧光猝灭的铜传感器研究

研究了过渡金属离子对荧光分子 1 萘胺二乙酸钠 (NADA)的荧光猝灭现象及其猝灭机理 ,并基于此建立铜离子传感体系。该铜离子传感器的检测限为8.2 7× 1 0 - 6mol/L ,定量检测范围为 2 .6 9× 1 0 - 5～ 1 .2 0× 1 0 - 4 mol/L。     

镧(Ⅲ)对铽(Ⅲ)-邻-氟苯甲酸-乙二胺体系荧光的增强及其分析应用

在pH 10.0的水溶液中,5.0×10-4 mol/L的La(Ⅲ)可使Tb(Ⅲ)-o-FBA(邻-氟苯甲酸)-EDA(乙二胺) 体系的荧光增强78倍.以1.0×10-9 mol/L的Tb(Ⅲ)试验,体系的最大荧光条件如下:o-FBA浓度为6.0×10-3 mol/L,EDA体积分数为1%,激发光波长为339 nm,测量的荧光发射波长为546 nm.实验表明,在上述条件下,Tb(Ⅲ)的浓度在5.0×10-10～2.0×10-7 mol/L范围与体系的荧光强度呈线性关系,据此建立了测定痕量铽的荧光光度分析法,测定的相对标准偏差为0.50%,Tb(Ⅲ)的检出限为5.0×10-11 mol/L.     

4,7-(氯磺酸基苯基)-1,10-菲啰啉-2,9-二羧酸-铕标记甲胎蛋白抗体

在合成BCPDA基础上 ,对甲胎蛋白抗体与BCPDA连接及与铕离子螯合条件进行了研究。BCPDA与甲胎蛋白抗体反应后 ,分离纯化最佳淋洗液为pH 9.1的 0 .1mol/L碳酸盐缓冲溶液 ,BCPDA用量为甲胎蛋白抗体量 (mol)的 12 0～ 16 0倍 ;反应时间为 30min。讨论了Eu3 + BCPDA AFP抗体螯合物的荧光光谱 ,最佳温育时间为6 0min ,体系pH值为 7.8的Tris HCl溶液。当Eu3 + 浓度为 10 -6mol/L时 ,BCPDA的检出限为 4 .3× 10 -11mol/L。     

铕敏化荧光法测定甲磺酸帕苏沙星

稀土Eu3+能与甲磺酸帕苏沙星形成络合物,并发出Eu3+的特征荧光.加入表面活性剂SDBS能大大增强体系的荧光强度,由此建立了表面活性剂敏化的Eu3+荧光探针测定甲磺酸帕苏沙星的方法.最佳测定条件为最大激发和发射波长分别是332和618 nm;pH=7.5;Eu3+浓度为1.2×10-5 mol/L,SDBS浓度为3.0×10-5 mol/L.甲磺酸帕苏沙星浓度在3.0×10-8～2.0×10-6 mol/L范围内与荧光强度线性关系良好,r=0.9993;检出限为1.0×10-9 mol/L.该方法用于甲磺酸帕苏沙星注射剂和人体血清以及尿样中的甲磺酸帕苏沙星的含量测定,结果令人满意.     

铕-镧-诺氟沙星-十二烷基磺酸钠稀土共发光体系的研究及分析应用

利用荧光光度法研究了铕-镧-诺氟沙星-十二烷基磺酸钠体系的稀土共发光效应,并对其作用机理进行了探讨.研究了本体系测定Eu3+的最佳条件,结果表明,体系的荧光强度与Eu3+的浓度在1.0×10-10～5.0×10-7 mol/L范围内呈良好的线性关系,其检出限为2.0×10-12 mol/L.采用标准加入法测定混合稀土样品中的Eu3+,结果令人满意.     

钇(Ⅲ)-莫西沙星配合物的荧光性质及分析应用

钇(Y3+)与莫西沙星(MoxifloxacinMXFX)形成的配合物能显著地增敏莫西沙星的荧光强度,据此,建立了测定莫西沙星的新方法。该方法的检出限为8.5×10-10mol/L;莫西沙星的浓度在1.0×10-8～1.0×10-6mol/L范围内与配合物体系的荧光强度呈良好的线性关系。对1.0×10-6mol/L莫西沙星平行测定12次,RSD为1.1%。该法可用于测定尿样中的莫西沙星。对荧光增强机理作了简要的探讨。     

Bi3+-Er3+ and Bi3+-Yb3+ Codoped Cs2AgInCl6 Double Perovskite Near-Infrared Emitters

Bi³⁺ and lanthanide ions have been codoped in metal oxides as optical sensitizers and emitters. But such codoping is not known in typical semiconductors such as Si, GaAs, and CdSe. Metal halide perovskite with coordination number 6 provides an opportunity to codope Bi³⁺ and lanthanide ions. Codoping of Bi³⁺ and Ln³⁺ (Ln=Er and Yb) in Cs₂AgInCl₆ double perovskite is presented. Bi³⁺-Er³⁺ codoped Cs₂AgInCl₆ shows Er³⁺ f-electron emission at 1540 nm (suitable for low-loss optical communication). Bi³⁺ codoping decreases the excitation (absorption) energy, such that the samples can be excited with ca. 370 nm light. At that excitation, Bi³⁺-Er³⁺ codoped Cs₂AgInCl₆ shows ca. 45 times higher emission intensity compared to the Er³⁺ doped Cs₂AgInCl₆. Similar results are also observed in Bi³⁺-Yb³⁺ codoped sample emitting at 994 nm. A combination of temperature-dependent (5.7 K to 423 K) photoluminescence and calculations is used to understand the optical sensitization and emission processes.     

Phosphine-catalyzed annulations of azomethine imines: allene-dependent [3 + 2], [3 + 3], [4 + 3], and [3 + 2 + 3] pathways

In this paper we describe the phosphine-catalyzed [3 + 2], [3 + 3], [4 + 3], and [3 + 2 + 3] annulations of azomethine imines and allenoates. These processes mark the first use of azomethine imines in nucleophilic phosphine catalysis, producing dinitrogen-fused heterocycles, including tetrahydropyrazolo-pyrazolones, -pyridazinones, -diazepinones, and -diazocinones. Counting the two different reaction modes in the [3 + 3] cyclizations, there are five distinct reaction pathways-the choice of which depends on the structure and chemical properties of the allenoate. All reactions are operationally simple and proceed smoothly under mild reaction conditions, affording a broad range of 1,2-dinitrogen-containing heterocycles in moderate to excellent yields. A zwitterionic intermediate formed from a phosphine and two molecules of ethyl 2,3-butadienoate acted as a 1,5-dipole in the annulations of azomethine imines, leading to the [3 + 2 + 3] tetrahydropyrazolo-diazocinone products. The incorporation of two molecules of an allenoate into an eight-membered-ring product represents a new application of this versatile class of molecules in nucleophilic phosphine catalysis. The salient features of this protocol--the facile access to a diverse range of nitrogen-containing heterocycles and the simple preparation of azomethine imine substrates--suggest that it might find extensive applications in heterocycle synthesis.     

Strong visible up-conversion emission in Tb3+, Tm3+ and Tb3+-Tm3+ co-doped tellurite glasses sensitized by Yb3+

Up-conversion luminescence characteristics under 975 nm excitation have been investigated with Tb3+/Tm3+/Yb3+ triply doped tellurite glasses. Here, green (547 nm: (5)D(4)-->(7)F(4)) and red (660 nm: (5)D(4)-->(7)F(2)) up-conversion (UC) luminescence originating from Tb3+ is observed strongly, because of the quadratic dependences of emission intensities on the excitation power. Especially, the UC luminescence was intensified violently with the energy transfer from the Tm3+ ions involves in the Tb3+ excitation. To the Tb3+/Tm3+/Yb3+ triply doped glass system, a novel up-conversion mechanism is proposed as follows: the energy of (3)G(4) level (Tm3+) was transferred to (5)D(4) (Tb(3+)) and the 477-nm UC luminescence of Tm3+ was nearly quenched.     

Pseudorotational dynamics of H3+ and Li3+

The origin of the pseudoprecession phenomenon is investigated through a computational study of the time evolution of H₃⁺ and Li₃⁺ by electron nuclear dynamics theory. In particular, the pseudorotation of both molecules is shown to induce a spatial rotation, which in turn leads to Coriolis coupling of the two orthogonal nuclear shape deformation modes. This effect is rooted in an anisotropy of the molecular ground state potential energy surface that is caused by the interaction between the D_3h ground state and a twofold degenerate first excited state. Computations are performed for a variety of vibrational energies. In addition, the impact of the anharmonicity of the ground state potential surface on the shape deformation modes and the coupling between them is discussed. © 2001 John Wiley & Sons, Inc. Int J Quantum Chem, 2001     

Spectroscopic properties of Er3+, Yb3 + and Er3 + /Yb3+ doped metaphosphate glasses

The absorption and emission spectroscopies of Er3+ doped and Er3+/Yb3+ codoped Ca(PO3)2, Sr(PO3)2 and Ba(PO3)2 glasses have been studied. From the Judd-Ofelt intensity parameters, the spontaneous emission probabilities of some relevant transitions and the radiative lifetimes of several excited states of Er3+ have been calculated. The decay curves of the Er3+ emission at 1.5 microm have been measured at different temperatures. The data have been fitted using a stretched exponential function and the obtained experimental lifetimes have been compared with the calculated radiative lifetimes. The difference between the experimental and calculated lifetimes is attributed to the presence of traces of OH groups in the host glasses. The absolute OH content in some glasses has been determined from the infrared spectra. The emission spectra at 1.5 microm of the Er3+ ion in the codoped glasses have been measured at different temperatures. The integrated emission intensities decrease significantly on passing from room temperature to 13 K, suggesting a temperature dependence of the rate of the energy transfer process between Yb3+ and Er3+.     

Energy transfer between Gd3+ and Sm3+ the effect of Gd3+ on quenching of Sm3+ and intensity parameters of Sm3+ in borate glasses

Intensity parameters of Sm³⁺ in borate glasses were obtained by fitting the oscillator strengths to the Judd-Ofelt formula and a study of energy transfer from gadolinium to samarium was performed. An increase of samarium fluorescence originating from the ${}^4\text{G}{}_{\mathrm{<mtext>5</mtext><mtext>2</mtext>}}$ level was observed in the presence of gadolinium, in the concentration range of 0.1–3 wt% samarium with gadolinium constant at 3 wt%. The intensity of samarium fluorescence on excitation at 273 nm increased by one order of magnitude in the presence of gadolinium. From the excitation spectrum of the double-doped glasses (Gd + Sm), it was deduced that energy absorbed by gadolinium is transferred from ${}^6\text{P}{}_{\mathrm{<mtext>7</mtext><mtext>2</mtext>}}$ gadolinium levels to the ${}^4\text{P}{}_{\mathrm{<mtext>3</mtext><mtext>2</mtext>}}$ and ${}^4\text{P}{}_{\mathrm{<mtext>5</mtext><mtext>2</mtext>}}$ samarium levels.The mechanism of this energy transfer was obtained by plotting the energy transfer probabilities as a function of samarium concentration. A linear dependence of $\text{η}{}_0\text{η}$ (η intensity of gadolinium in the presence of samarium) versus square of concentration of Sm + Gd is obtained. From this it is concluded that the transfer is of electric-multipolar type, mainly dipole-dipole. A small increase (about 10%) of fluorescence of samarium in the presence of gadolinium excited at levels where no energy transfer can take place is attributed to the fact that the quenching of samarium occurring by the cross relaxation $\text{(}{}^4\text{G}{}_{\mathrm{<mtext>5</mtext><mtext>2</mtext>}}\text{→}{}^6\text{F}{}_{\mathrm{<mtext>9</mtext><mtext>2</mtext>}}\text{) (}{}^6\text{H}{}_{\mathrm{<mtext>5</mtext><mtext>2</mtext>}}\text{→}{}^6\text{F}{}_{\mathrm{<mtext>9</mtext><mtext>2</mtext>}}\text{)}$ is suppressed by the presence of gadolinium as seen from concentration dependence of samarium doped glasses compared to double-doped glasses.     

Er3+-Tm3+-Yb3+ tri-doped CaMoO4 upconverting phosphors in optical devices applications

The structural and optical properties of the Er³⁺-Tm³⁺-Yb³⁺codoped CaMoO₄ phosphors prepared by chemical route have been explored. The crystalline structures of the prepared phosphors have been investigated with the help of X-ray diffraction analysis. The presence of different vibrational modes and absorption bands arising due to the transitions from the ground state to different excited states of rare earth ions have been identified using the Raman and UV-VIS-NIR absorption spectra of the developed phosphor, respectively. The concentration quenching effect on the luminescence property of the prepared materials has been explained in detail. The upconversion luminescence property of the Er³⁺-Tm³⁺-Yb³⁺codoped CaMoO₄ phosphor annealed at different temperatures under 980 nm and 808 nm excitations have been reported. The energy transfer Er³⁺ → Tm³⁺, Yb³⁺ → Er³⁺ and Tm³⁺ has been found to be responsible for efficient UC emission. The dipole-dipole interaction is observed to be responsible for the concentration quenching of the luminescence intensity. The effect of annealing temperature on the upconversion luminescence property has been explained in detail. The results suggest that the developed tri-doped phosphor may be suitable in making the efficient NIR to visible upconverter and lighting based optical devices.     

Tb~(3+)在YAG中的发光及Tb~(3+)与Tm~(3 +)间的能量传递

采用溶胶 -凝胶方法合成了系列化合物 (Y1 -x- yTbxTmy) 3Al5O1 2 ,研究了Tb3+在该化合物中的发光及其浓度对发光性质的影响 ,以及Tb3+与Tm3+间的能量传递现象。     

沉淀法制备Sm3+,Er3+与Nd3+一次共掺杂的BaTiO3基半导体陶瓷电容器

在共沉淀法的基础上,通过双施主不同浓度的Nd3+和Sm3+,Er3+(4.0%～5.0%)掺杂,研究了BaTiO3基表面型陶瓷电容器的电性能,结果表明,Sm3+和Er3+的掺杂可以提高居里温度,但使介电常数降低,其含量为25%时可获得绝缘电阻500 MΩ左右,C/S为0.5895μf·cm-2电性能参数.