铕(Ⅲ)荧光增敏体系在微乳液中的发光性质和荧光衰减动力学研究

利用稳态和瞬态光谱方法研究了不同铕离子发光体系中各种因素对铕离子发光性质的影响.通过吸收和激发光谱的变化分析了稀土离子Gd³⁺对Eu³⁺增敏机理,并从荧光衰减动力学角度证明了主配体噻吩甲酰三氟丙酮(TTA)、协配体邻啡咯啉(Phen)、稀土离子Gd³⁺和表面活性剂TX-100对铕离子发光的增敏作用.4种发光体系Eu³⁺/Gd³⁺/TTA/Phen/TX-100,Eu³⁺/TTA/Phen/TX-100,Eu³⁺/Gd³⁺/TTA/Phen和Eu³⁺/Gd³⁺/TTA/TX-100中铕离子⁵D₀态的发光寿命依次为980>670>400>260μs,而且存在铕离子⁵D₁到⁵D₀的传能过程.在发光越强的体系中,⁵D₁的衰减越慢,相应地⁵D₀的上升时间也就越长.研究结果表明,在最佳发光体系中既存在分子内的能量转移,又存在分子间的能量传递.     

稀土离子跨人血红细胞膜的荧光法研究

采用Fura-2荧光浓度指示剂对红细胞的稀土跨膜作用进行了系列研究.结果表明,稀土离子不能通过完整的红细胞膜进入细胞内.通过与离子载体实验相对照,发现细胞ATP耗竭后,低浓度的稀土离子(5×10^-6mol/L)不能跨膜进入ATP-耗竭红细胞.KCl去极化及加入电压依赖性钙通道刺激剂Bay-K8644对稀土离子的跨膜也没有促进作用.在Ca²⁺内流正常的情况下,低浓度稀土离子(5×10^-6mol/L)对钙离子内流无影响.增大稀土离子浓度到5×10^-4mol/L,用显微镜观察此时红细胞已开始溶血.在模拟胞内离子组分的缓冲液中(pH=7.05),比较了La³⁺,Eu³⁺和Ca²⁺对Fura-2的敏感程度.此条件下Fura-2对La³⁺和Eu³⁺的检测限分别为10-12和10-14mol/L,对Ca²⁺的检测限为10-8mol/L,并测得Fura-2-La³⁺(Eu³⁺)的络合比为1∶1,表观离解常数为1.7×10^-12和4.95×10^-14mol/L,表明用此法检测稀土离子跨膜行为相当灵敏有效.     

KMnF3的熔盐法合成及掺铕体系的发光性质

采用简单的熔盐法合成了KMnF₃单相样品及稀土离子铕掺杂的KMnF₃（KMnF₃：Eu）荧光样品. X射线粉末衍射（XRD）表征结果显示,KMnF₃属立方晶系,为AMF₃型钙钛矿结构氟化物. 对样品KMnF₃：Eu的发光性质进行了研究,荧光光谱分析结果表明,Mn²⁺,Eu²⁺与Eu³⁺这3个发光中心共存于KMnF₃：Eu体系中. 讨论了改变掺入Eu离子的摩尔分数对Mn²⁺,Eu²⁺以及Eu³⁺发光强度的影响.     

稀土元素的电分析化学研究(Ⅰ)——铕的极谱研究

用交流极谱法比较了Eu⁺³离子在NH₄SCN、EDTA-NaCl、DTPA-NaCl三种底液中的极谱行为,其中以在DTPA-NaCl底液中的极谱可逆性为最好。使用DTPA-NaCl底液测定Eu⁺³的最宜条件为:pH>6.5,NaCl浓度>0.3M,DTPA浓度略大于溶液中全部可与DTPA络合的金属离子的总浓度。在此条件下,用交流极谱或单扫示波极谱法测定Eu⁺³的下限为2×10^-6M,用微分脉冲极谱法测定为2×10^-7M。其他稀土离子不干扰。还测定了某些稀土氧化物样品中少量的Eu,得到满意的结果。     

掺铥硫氧化钇的特殊余辉性质

迄今为止,稀土长余辉磷光体已见文献或专利公开报道的激活离子主要有适于紫外光激发的三价铈离子(Ce³⁺)和三价镨离子(Pr³⁺)、适于可见光激发的铕离子(Eu³⁺和Eu²⁺)及钐离子(Sm³⁺,Sm²⁺),尚未涉及到铥离子Tm³⁺或Tm²⁺.我们在Tm³⁺离子激活的硫氧化钇体系Y₂O₂S:Tm³⁺中发现了长余辉荧光特性.特别是在该磷光体中还发现了一种非常特殊的余辉现象.     

稀土掺杂氟化镁钾纳米晶的合成及其光谱特性

采用微乳液法合成了Eu²⁺,Ce³⁺单掺和双掺KMgF₃纳米晶,分析了样品的结构与形态. 结果表明,所合成的样品均为单相,颗粒粒度分布均匀. 讨论了光谱特性并与高温固相法合成的产物作了对比. 研究发现,在KMgF₃纳米晶双掺体系中,由于Eu²⁺和Ce³⁺竞争吸收激发能,只能观察到Ce³⁺的发射带; 而在KMgF3多晶共掺体系中,因为存在Ce³⁺→Eu²⁺能量传递过程,只能观察到Eu²⁺的发射峰.     

尖吻蝮蛇毒抗凝血因子Ⅱ的稀土离子荧光探针研究

尖吻蝮蛇毒抗凝血因子(ACF)分子中有两个钙离子结合位点,钙离子对ACF的内源荧光有增强作用,稀土离子(Nd³⁺,Sm³⁺,Eu³⁺,Gd³⁺和Tb³⁺)能取代ACF分子中的钙离子,并对ACF的内源荧光有不同程度的猝灭作用,其中Tb³⁺接受ACF分子中Trp残基传递的能量后,特征荧光增强.稀土离子与ACF荧光滴定表明,ACF分子中有两个稀土离子结合位点,稀土离子和钙离子在ACF分子中两个结合部位是共同的竞争结合部位.ACF与不同稀土离子之间有相近的表观结合常数K₁或K₂.Tb³⁺与RE³⁺(RE=Nd,Sm,Eu或Gd)间线性自由能关系表明,稀土离子与ACF结合时,没有明显的空间效应.ACF分子中的两个结合位点在结构上都有较大的柔性,这种结构柔性为钙离子在ACF与活化凝血因子X的结合反应中起到的促进作用提供了结构基础.     

稀土离子对钙调蛋白与单克隆抗体分子识别的影响

分别采用酶联免疫吸附(ELISA)法和荧光标记技术比较了Ca²⁺,La³⁺,Eu³⁺和Yb³⁺离子对钙调蛋白与单克隆抗体2C3之间分子识别的影响.结果表明,金属离子与钙调蛋白作用后会诱导其发生不同的构象变化,并进一步影响到钙调蛋白与单克隆抗体2C3分子之间的结合强度.当钙调蛋白分别与La³⁺,Eu³⁺,Yb³⁺作用后,它与单抗2C3分子之间的解离常数为(26.8±2.5),(21.8±3.4)和(64.8±5.1)nmol/L,而结合Ca²⁺前后的钙调蛋白与单抗分子的解离常数分别为(177.2±2.8)和(157±4.2)nmol/L.这一结果表明,稀土离子诱导钙调蛋白发生的构象变化明显不同于钙离子的作用,这种差异可能是稀土与钙离子对钙调蛋白调控作用表现出差别的原因.     

Hf4+共掺NaYF4:Yb/Tm提高上转换发光性能研究

利用X射线多晶衍射仪、场发射扫描电镜、场发射透射电镜、X射线光电子能谱和荧光光谱仪对相近半径离子Hf⁴⁺和Zr⁴⁺共掺六方NaYF₄:Yb³⁺/Tm³⁺的结构、形貌和上转换发光性能进行研究.结果表明Hf⁴⁺和Zr⁴⁺离子共掺六方NaYF₄:Yb³⁺/Tm³⁺可有效调控晶场的不对称性, Hf⁴⁺相对于Zr⁴⁺是个更好的掺杂离子,它在调控晶场的同时还参与Tm³⁺离子上转换发光的能量传递过程,明显提高了短波500 nm以下发射带的荧光强度;而Zr⁴⁺离子仅扮演晶场调控角色而未能参与稀土离子Tm³⁺的上转换发光过程, Tm³⁺离子小于500 nm短波发射带的荧光强度没有得到明显的提高,仅提高802 nm发射带的荧光强度.该研究发现Hf⁴⁺可作为蓄能离子参与稀土离子的上转换发光过程,有助于将Hf⁴⁺作为蓄能离子和晶格操纵工具用于设计和制备其它高性能的稀土上转换发光材料.     

铕(Ⅲ)激活的磷酸镧发光性质研究

LaPO₄:Eu³⁺的发射光谱包含较强的Eu³⁺⁵D_o→⁷F₁跃迁发射和较弱的⁶D₁→⁷F₁跃迁发射。主发射峰583nm,对应于Eu³⁺5D_o→⁷F₁跃迁.通过对Eu³⁺的两种跃迁发射强度及荧光寿命和Eu³⁺浓度关系的测定和理论分析,探讨了发光中心Eu³⁺离子同的交叉弛豫和能量迁移机理。     

共振喇曼光谱研究稀土离子Er3对肌红蛋白结构的影响

随着稀土金属开发应用的不断深入 ,它的安全性已引起人们的广泛关注 .Evans[1]曾报道稀土化合物由于其类 Ca2 + 性导致各种负面生物效应 ,包括影响心血管功能及溶血 ,然而有关稀土离子影响血红素蛋白结构的研究尚很少见报道 .肌红蛋白由含 1 5 2个残基的单一多肽链 (珠蛋白 )和血红素组成 .在生物体中 ,它为肌肉组织贮存氧 ,以供细胞呼吸的需要 ,因此它在人体中具有极其重要的生理作用 .研究稀土离子对肌红蛋白的影响对了解稀土离子降低血红素蛋白载氧能力的作用机理具有实际意义[2 ] .由于血红素在可见和近紫外区有很强的吸收带 ,以氩离子…     

Fourier transform Raman approach to structural correlation in hemoglobin derivatives.

In order to obtain information on the structural aspects of hemoglobin (Hb), Fourier transform Raman (FT-R) measurements on various ferrous, ferric derivatives and nickel reconstituted Hb (NiHb) has been made. FT-R spectra for these derivatives were obtained by laser excitation in the near infrared region (NIR) (1064 nm) whereby the wave-number region (600-1700 cm-1) related to both porphyrin ring modes and some globin modes were monitored. Comparison of various modes was made based on previous resonance Raman (RR) results. The wave-number shifts with respect to changes in oxidation state and spin state are very similar to those observed by RR. Additional bands at 1654, 1459, and 1003 cm-1 for deoxyHb and at 1656, 1454, and 1004 cm-1 for oxy Hb can be correlated to globin modes. The shift in the position of these bands for the binding of oxygen can be related to changes in conformation during the transformation. The presence of two distinct sites in NiHb could be monitored by the use of FT-R technique.     

First example of low-valence ion substitution in Ln5O(OPri)13: mixed-valence europium oxoalkoxide [EuIII4EuIIO(OPri)12(HOPri)]HOPri

The novel mixed-valence alkoxide [Eu3+(4)Eu2+O(OPri)12(HOPri)]HOPri (1) has been prepared and structurally and spectroscopically characterized. The three synthesis routes (i) metathesis of 4EuCl3, EuI2, and 14KOPri combined with hydrolysis with 1H2O, (ii) oxidation of 5[Eu4(OPri)10(HOPri)3]2HOPri with 1.5O2, and (iii) reduction of Eu5O(OPri)13 with 0.8[Eu4(OPri)10(HOPri)3]2HOPri all yielded pure 1, whereas (iv) reduction of Eu5O(OPri)13 with 0.36-0.5 mol of europium metal produced impure 1. The compound, having the average Eu oxidation number +2.8, is very sensitive toward further oxidation to Eu5O(OPri)13 and is part of a redox series of europium 2-propoxides with average oxidation states +2.5, +2.8, and +3. The square pyramidal molecular structure, containing an oxo-oxygen atom in the basal plane, is similar to that of the well-known Ln5O(OPri)13; the main difference is the substitution of an Eu3+(-)OPri pair for an Eu2+(-)HOPri pair in the basal plane. Fourier transform infrared (FT-IR) and UV-visible spectroscopy showed that the solid-state structure was retained on dissolution in hexane and toluene-HOPri. The compound was further characterized by differential scanning calorimetry and solubility studies.     

Eu0.5RE0.5Fe0.5Mn0.5O3的57Fe Msosbauer谱研究

利用固相反应合成了Eu0.5RE0.5Fe0.5Mn0.5O3(RE=La,Pr,Nd,Sm,Eu,Gd,Tb,Dy,Ho,Er,Tm,Yb,Y)等化合物。测量了其XRD谱及57FeMssbauer谱。实验发现,随着RE原子序数的增加,样品的晶胞体积减小,Fe在化合物中处于Fe3+的高自旋状态,57Fe的四极裂矩与样品的畸变参数D成线性关系。     

Eu_（0．5）RE_（0．5）Fe_（0．5）Mn_（0．5）O_3的~（57）Fe Msosbauer谱研究

利用固相反应合成了Ｅｕ_（０．５）ＲＥ_（０．５）Ｆｅ_（０．５）Ｍｎ_（０．５）Ｏ_３（ＲＥ＝Ｌａ，Ｐｒ，Ｎｄ，Ｓｍ，Ｅｕ，Ｇｄ，Ｔｂ，Ｄｙ，Ｈｏ，Ｅｒ，Ｔｍ，Ｙｂ，Ｙ）等化合物。测量了其ＸＲＤ谱及~（５７）ＦｅＭｓｓｂａｕｅｒ谱．实验发现，随着ＲＥ原子序数的增加，样品的晶胞体积减小，Ｆｅ在化合物中处于Ｆｅ~（３＋）的高自旋状态，~（５７）Ｆｅ的四极裂矩与样品的畸变参数Ｄ成线性关系。     

Eu3+在碱土金属卤磷酸盐中的格位对称性及电荷迁移态

在254nm紫外光激发下研究了Eu~(3+)在Sr_3Ca_2(PO_4)_3Cl基质中的发光光谱.以Eu~(3+)为结构探针测定了Eu~(3+)所处晶格的点对称性.研究了M_5(PO_4)_3X(M=Ca,Sr,Ba;X=F,Cl,Br)基质组成改变对Eu~(3+)电荷迁移态的影响,以及温度对Ca_5(PO_4)_3Cl:Eu~(3+)发光强度的影响.     

掺杂铕和铽的卤硼酸盐荧光体的制备及光谱特征

采用高温固相法在空气中合成了一系列掺杂稀土离子的卤硼酸盐荧光体, 研究了其发光性质和基质组成对稀土离子共掺杂的荧光体发光性质的影响. 研究结果表明, 在Eu3+和Tb3+共掺杂的体系中存在电子转移, 因此出现了Eu3+, Eu2+和 Tb3+共存于同一基质共同发射的现象. Ce3+对Eu2+和Tb3+具有敏化作用, 可增强其发射强度. 基质的组成对稀土离子的发射峰位和发射强度有明显影响.     

Sr2SiO4:Eu3+发光材料的制备及其光谱特性

采用溶胶-凝胶法制备了Sr2SiO4:Eu3+发光材料. 测量了Sr2SiO4:Eu3+材料的激发与发射光谱, 发射光谱主峰位于618 nm处;监测618 nm发射峰时, 所得激发光谱主峰分别为320、397、464 和518 nm. 研究了Sr2SiO4:Eu3+材料在618 nm的主发射峰强度随Eu3+浓度的变化情况. 结果显示, 随Eu3+浓度的增大, 发射峰强度先增大; 当Eu3+浓度为7%时(x), 峰值强度最大; 而后随Eu3+浓度的增大, 峰值强度减小. 在Eu3+浓度为7%的情况下, 研究了电荷补偿剂Li+的掺杂浓度(x(Li+))对Sr2SiO4:Eu3+材料发射光谱强度的影响. 结果显示, 随x(Li+)的增大, 材料发射光谱强度先增大后减小, 当x(Li+)为8%时, 峰值强度最大.     

Theoretical approach to fluorine substitution in X2NO and X2CN free radicals. Comparison between ab initio UHF and RHF + perturbation treatments

Non-empirical calculations have been performed to analyze the effects of fluorine substitution on the geometry and electronic properties of two series of π and σ radicals. Both UHF and RHF + perturbation methods have been used and the results are compared as a function of the basis set quality. As concerns geometry and spin-free electronic properties the results are independent of the UHF or RHF formalism, but highly sensitive to the basis set. The STO-3G basis is unable to reproduce even general trends. Polarization functions always play a relevant role and correlation effects seem not negligible at least for fluorine-containing radicals. The molecular shape of π radicals changes from a planar to a pyramidal geometry when increasing the electronegativity of the substituents. On the contrary, σ radicals always remain planar. Unprojected UHF spin densities are closer to the RHF + perturbation results for small spin contamination (X₂NO). On the contrary, it is the projected UHF spin density which is in better agreement with the RHF + perturbation value for large spin contamination (X₂CN). No simple correlation can be found between spin densities and gross atomic spin populations. For H₂NO the spin density at nitrogen is smaller than at the oxygen nucleus, but substitution may enhance or reverse this trend.     

Optical properties of nanocrystalline Y2O3:Eu depending on its odd structure

The structure of nanocrystalline Y2O3:Eu prepared by a combustion reaction was analyzed by XRD and high-resolution electron microscopy. Compared with a large-scale particles, 5-nm Y2O3:Eu particles presented as distorted crystallite and rough surfaces. Luminescent and absorption properties of nano-Y2O3:Eu showed remarkably particle size effects. At Y2O3:Eu particle sizes smaller than 10 nm some new results were observed: (a) a red shift of the charge-transfer-state absorption; (b) new emission bands of Eu3+ in the 5D0 --> 7F2 region; (c) luminescent decay of energy level 5D0 of Eu3+ turning to a two-step exponential; and (d) a pronounced increase in quenching concentration and much lower phonon density compared with those of the bulk material. All these phenomena can be attributed to the effect of the softened lattice and surface state of the nanomaterial. The latter was confirmed by stronger excitation by the host absorption after the surface modification.