Gd2(CO3)3:Eu@SiO2@APTES磁性-荧光双功能核壳微球的制备与性能

采用尿素均相沉淀法和Stöber法制备了氨基化SiO₂修饰的Gd₂(CO₃)₃:Eu顺磁性-荧光双功能微球。用扫描电镜(SEM)、红外光谱(IR)、X-射线粉末衍射(XRD)等测试手段对微球的结构和颗粒特征进行了分析。结果表明:微球为核壳结构,其Gd₂(CO₃)₃:Eu核平均直径为150nm左右,SiO₂壳层的厚度大约为30nm,分散性良好。磁性测试显示微球拥有良好的顺磁性,荧光光谱表明,在396nm紫外光激发下,微球在613nm发射较强荧光,属于Eu³⁺的特征发射,同时微球能成功标记NCIH460肺癌细胞,MTT毒性测试表明该法制备的双功能微球在100~400μg·mL^-1的浓度范围内无毒,表明其在生物应用方面的潜在应用价值。     

水热法制备多层核壳结构Gd2O3∶Eu3+空心微球

以稀土硝酸盐-葡萄糖的混合溶液作为前驱体,采用一步水热法和随后的热处理得到了多层核壳结构Gd₂O₃∶Eu³⁺空心微球,并用X-射线衍射(XRD)、场发射扫描电镜(FESEM)、透射电镜(TEM)、X-射线能量色散光谱(EDS)和荧光光谱等测试手段对所得样品进行了表征。结果表明：所得空心球样品为纯的立方相的Gd₂O₃。具有规则的多层核壳空心结构,空心球的直径在2~3 μm左右,壁厚约为100 nm,并且Gd₂O₃∶Eu³⁺空心球是由尺寸约为30 nm的球形纳米颗粒自组装而成。样品中含有Gd、Eu、O元素。该空心球样品具有强的Eu³⁺的特征红光发射以及长的荧光寿命,可以用来作为时间分辨荧光标记物。     

多级结构Mg3B2O6:Eu3+花状微球的制备、表征及其发光性能

以硝酸镁(Mg(NO₃)₂·6H₂O)和硼砂(Na₂B₄O₇·10H₂O)为原料,稀土元素Eu³⁺为激活剂,采用聚乙烯吡咯烷酮(PVP)辅助共沉淀法得到前驱体,并通过焙烧制备了多级结构Mg₃B₂O₆:Eu³⁺花状微球。通过XRD、SEM、TEM以及荧光光谱等手段分别对前驱体煅烧产物的结构、形貌、组成和荧光特性进行了表征。实验表明,在波长为393 nm激发光的激发下,所得到的产品在612 nm处有明显的特征发射峰,对应于Eu³⁺的(⁵D₀→⁷F₂)特征跃迁发射。这一荧光性质使得该材料在荧光灯、显示系统和光电设备应用中具有广阔的前景。同时我们还探讨了微球的形态、Eu³⁺的掺杂量及焙烧温度对花状微球荧光性能的影响。     

多级结构Mg3B2O6: Eu3+花状微球的制备、表征及其发光性能

以硝酸镁(Mg(NO₃)₂·6H₂O)和硼砂(Na₂B₄O₇·10H₂O)为原料, 稀土元素Eu³⁺为激活剂, 采用聚乙烯吡咯烷酮(PVP)辅助共沉淀法得到前驱体, 并通过焙烧制备了多级结构Mg₃B₂O₆: Eu³⁺花状微球。通过XRD、SEM、TEM以及荧光光谱等手段分别对前驱体煅烧产物的结构、形貌、组成和荧光特性进行了表征。实验表明, 在波长为393 nm激发光的激发下, 所得到的产品在612 nm处有明显的特征发射峰, 对应于Eu³⁺的(⁵D₀→⁷F₂)特征跃迁发射。这一荧光性质使得该材料在荧光灯、显示系统和光电设备应用中具有广阔的前景。同时我们还探讨了微球的形态、Eu³⁺的掺杂量及焙烧温度对花状微球荧光性能的影响。     

同轴静电纺丝技术制备Y2O3:Eu3＋@SiO2豆角状纳米电缆与表征

采用同轴静电纺丝技术, 以氧化钇、氧化铕、正硅酸乙酯(C₈H₂₀O₄Si)、无水乙醇、PVP和DMF为原料, 成功制备出大量的Y₂O₃:Eu^3＋@SiO₂豆角状纳米电缆. 用TG-DTA, XRD, SEM, TEM和荧光光谱等分析技术对样品进行了系统地表征． 结果表明, 得到的产物为Y₂O₃:Eu^3＋@SiO₂豆角状纳米电缆, 以无定型SiO₂为壳层, 晶态Y₂O₃:Eu^3＋球为芯, 电缆直径约为200 nm, 内部球平均直径约150 nm, 壳层厚度约为25 nm, 电缆长度＞300 μm. 纳米电缆内部为球状结构, 沿着纤维长度方向有序排列, 形貌均一. Y₂O₃:Eu^3＋@SiO₂豆角状纳米电缆在246 nm紫外光激发下, 发射出Eu^3＋离子特征的波长为614 nm的明亮红光. 对其形成机理进行了初步讨论.     

红色荧光粉CePO4-6LaPO4@4SiO2:Eu3+的发光特性

采用溶胶凝胶-高温固相法制备CePO₄-6LaPO₄@4SiO₂∶Eu³⁺荧光粉,通过XRD、TEM、EDS、IR以及激发光谱和发射光谱对荧光粉的结构和发光性能进行了表征。XRD和EDS结果证明了目标产物,其由晶态的LaPO₄、CePO₄和非晶态的SiO₂构成;TEM图显示样品形貌为不规则形状,并且显示CePO₄-6LaPO₄@4SiO₂∶Eu³⁺荧光粉形成核壳结构;HRTEM图可以清楚地看出晶格条纹的形成;IR谱图显示结果与XRD和EDS的分析结果一致;荧光光谱图显示：在466 nm激发下,CePO₄-6LaPO₄@4SiO₂∶Eu³⁺荧光粉在615 nm处出现属于Eu³⁺的⁵D₀→⁷F₂跃迁的强烈红光发射。     

Fe3O4@SiO2@mTiO2介孔多功能纳米复合颗粒的制备及载药能力

以溶剂热法制备氨基功能化的Fe₃O₄纳米颗粒为磁核,结合溶胶-凝胶法和模板法在其表面先后包覆上致密的SiO₂层和介孔TiO₂层,制备了磁性-发光-微波热转换性-介孔结构为一体的多功能核-壳结构纳米复合颗粒,并对其结构、性能及载药能力进行了研究。XRD分析表明:Fe₃O₄表面包覆上了无定形结构的SiO₂和TiO₂。TEM照片表明:所得的纳米复合颗粒具有明显的核壳结构和完美的球形,构成核的Fe₃O₄颗粒的尺寸在40~50 nm之间,Fe₃O₄@SiO₂@mTiO₂核壳结构纳米复合颗粒的尺寸为60~70 nm,壳层厚度约10 nm,并可观察到壳层中清晰的孔状结构。磁性、荧光光谱和微波热转换特性分析表明:该复合颗粒同时具有良好的发光性、磁性和微波热转换特性。N₂气吸附及药物负载率分析表明,该复合颗粒具有较高的比表面积(640 m²·g^-1)和介孔结构(孔径约2.8 nm)并且具有较高的药物负载率。     

新型铕配合物二氧化硅荧光纳米粒子DPPDA-Eu3+/SiO2的制备与表征

本文首先合成配位体4,7-二苯基-1,10-菲罗啉-2,9-二羧酸(DPPDA,C₂₆H₁₆N₂O₄)及铕配合物DPPDA-Eu³⁺((C₂₆H₁₆N₂O₄)₂Eu·15H₂O),然后采用反相微乳液法,通过正硅酸乙酯和3-氨丙基三甲氧基硅烷的共水解、聚合作用成功制备出表面带氨基的二氧化硅包裹铕配合物DPPDA-Eu³⁺的核壳型荧光纳米颗粒DPPDA-Eu³⁺/SiO₂。利用透射电子显微镜、荧光光谱、紫外-可见光谱等手段进行表征,并进行了光稳定性、荧光泄露与氨基测定等实验,结果表明所制备的纳米粒子呈规则球状,大小均匀,粒径为80±8 nm,具有良好的单分散性和光稳定性,不易发生荧光分子从二氧化硅壳层中泄露,纳米粒子表面带有氨基,可不需要进行表面修饰而直接与生物分子反应。该纳米粒子可望作为一种新型的稀土荧光探针应用于时间分辨荧光免疫分析、生物芯片及生物传感器等。     

Li4SrCa (SiO4)2:Eu3+红色荧光粉的合成及其发光性能

采用硅酸盐作为基质材料,通过高温固相法合成了Li₄SrCa（SiO₄）₂：Eu³⁺红色荧光粉。通过X射线粉末衍射、X射线光电子能谱、透射电镜和荧光光谱,对所得样品的物相、形貌及其发光性能进行了表征分析。结果表明,掺入Eu³⁺后,Li₄SrCa（SiO₄）₂的晶体结构并没有发生改变。在393 nm光激发下,荧光粉的荧光光谱中693 nm处发射峰强度最强。以693 nm作为监测波长,荧光激发峰分别为361 nm（⁷F₀→⁵D₄）、375 nm（⁷F₀→⁵G₃）、413 nm（⁷F₀→⁵D₃）、393 nm（⁷F₀→⁵L₆）和464 nm（⁷F₀→⁵D₂）,即样品对近紫外和蓝光有较好的吸收。利用发射光谱研究了Eu³⁺掺杂浓度（物质的量分数）对荧光粉发光强度的影响。当Eu³⁺的掺杂浓度x=0.10时,样品发射强度最强,发射红光,其色坐标为（0.637 5,0.353 7）。通过Dexter强度与浓度关系分析了浓度猝灭机制。     

Tm3+/Er3+/Ho3+共掺SiO2-Bi2O3-AlF3-BaF2玻璃发光性能

采用高温熔融法制备了Tm³⁺/Er³⁺/Ho³⁺共掺的铋硅酸盐50SiO₂-40Bi₂O₃-5AlF₃-5BaF₂玻璃。研究了在808 nm激光器（Laser Diode）激发下Tm³⁺/Er³⁺/Ho³⁺共掺的铋硅酸盐在2 060 nm处的发光性能,同时测试及分析了该铋硅酸盐玻璃的差热特性、吸收光谱及荧光光谱。根据吸收光谱以及Judd-Oflet理论,计算了Ho³⁺的Judd-Oflet强度参数Ω_t（t=2,4,6）以及Tm³⁺/Er³⁺/Ho³⁺相应的吸收截面。铋硅酸盐玻璃中,Tm₂O₃、Er₂O₃和Ho2O3掺杂浓度分别为0.75%、1.0%和0.5%时,2 060 nm处Ho³⁺∶⁵I₇→⁵I₈发射峰强度达到最大。对Tm³⁺/Er³⁺/Ho³⁺ 3种离子的光谱性质和离子间可能存在的能量传递也做了分析。Ho³⁺在1 953 nm处的最大吸收截面σ_abs为9.08×10^-21 cm²,在2 060 nm处的最大发射截面σem为11.68×10^-21 cm²,辐射寿命τ_mea为2.75 ms,具有良好的增益效应σ_emτ（3.212×10^-20 cm^-2·ms）。     

Sm2O3Ga2O3 and Gd2O3Ga2O3 phase diagrams

Four definite compounds exist in the Sm₂O₃Ga₂O₃ binary phase diagram, namely: Sm₃GaO₆, Sm₄Ga₂O₉, SmGaO₃, and Sm₃Ga₅O₁₂. The $\text{3}\text{1}$ compound is orthorhombic (space group Pnna - Z.4) with the cell parameters: a = 11.40₀Å, b = 5.51₅Å, c = 9.07Å and belongs to the oxysel family. Sm₃GaO₆ and SmGaO₃ melt incongruently at 1715 and 1565°C; Sm₄Ga₂O₉ and Sm₃Ga₅O₁₂ have a congruent melting point at 1710 and 1655°C. With regard to the Gd₂O₃Ga₂O₃ system three definite compounds have been identified: Gd₃GaO₆, Gd₄Ga₂O₉, and Gd₃Ga₅O₁₂. Only the garnet melts congruently at 1740°C with the following composition: Gd_3.12Ga_4.88O₁₂. Gd₃GaO₆, and Gd₄Ga₂O₉ melt incongruently at 1760 and 1700°C. GdGaO₃ is only obtained by melt overheating which may yield an equilibrium or a metastable phase diagram.     

Garnet-perovskite transformations in the Sm2O3Ga2O3 and Gd2O3Ga2O3 systems

The effect of heating garnet melts to various temperatures has been investigated. The previously reported decomposition of the garnet phase due to loss of Ga₂O₃ was corroborated. However, it was also observed that when gallium oxide loss is prevented and the maximum temperature of the melt exceeds a critical value, phase separation of garnet to perovskite and β-gallium oxide occurs:

$\text{RE}{}_3\text{Ga}{}_5\text{O}{}_{12}\text{?3RE}\text{GaO}{}_3\text{+}\text{Ga}{}_2\text{O}{}_3$

.The reverse reaction will occur by reheating the two-phase mixture to the garnet melting point.     

Phase transitions in Ca3(BN2)2 and Sr3(BN2)2

α-Ca₃(BN₂)₂ crystallizes in the cubic system (space group: ) with one type of calcium ions disordered over of equivalent (8c) positions. An ordered low-temperature phase (β-Ca₃(BN₂)₂) was prepared and found to crystallize in the orthorhombic system (space group: Cmca) with lattice parameters: , , and . Structure refinements on the basis of X-ray powder data have revealed that orthorhombic β-Ca₃(BN₂)₂ corresponds to an ordered super-structure of cubic α-Ca₃(BN₂)₂. The space group Cmca assigned for β-Ca₃(BN₂)₂ is derived from by a group-subgroup relationship.DSC measurements and temperature-dependent in situ X-ray powder diffraction studies showed reversible phase transitions between β- and α-Ca₃(BN₂)₂ with transition temperatures between 215 and 240 °C.The structure Sr₃(BN₂)₂ was reported isotypic with α-Ca₃(BN₂)₂ () with one type of strontium ions being disordered over of equivalent (2c) positions. In addition, a primitive () structure has been reported for Sr₃(BN₂)₂. Phase stability studies on Sr₃(BN₂)₂ revealed a phase transition between a primitive and a body-centred lattice around 820 °C. The experiments showed that both previously published structures are correct and can be assigned as α-Sr₃(BN₂)₂ (, high-temperature phase), and β-Sr₃(BN₂)₂ (, low-temperature phase).A comparison of Ca₃(BN₂)₂ and Sr₃(BN₂)₂ phases reveals that the different types of cation disordering present in both of the cubic α-phases () have a directing influence on the formation of two distinct (orthorhombic and cubic) low-temperature phases.     

Interactions of Cr2S3 with GeS2 and Cu2GeS3

The interactions in the GeS₂-Cr₂S₃ and Cu₂GeS₃-Cr₂S₃ sections were studied by differential thermal analysis and X-ray powder diffraction. The GeS₂-Cr₂S₃ section was shown to be quasi-binary, with a degenerate eutectic; no ternary compound was formed. In the Cu₂GeS₃-Cr₂S₃ section, a quaternary phase of variable composition having a homogeneity range of 69–75 mol % Cr₂S₃ crystallized in the cubic system. The samples of this composition are spin glasses with freezing temperatures of 20–25 K.     

Syntheses and structures of three new scandium selenites: Sc2(SeO3)3·H2O, Sc2 (SeO3)3·3H2O and CsSc3(SeO3)4 (HSeO3)2·2H2O

Three new hydrated scandium selenites have been hydrothermally synthesized as single crystals and structurally and physically characterized. Sc₂(SeO₃)₃·H₂O crystallizes as a new structure type containing novel ScO₇ pentagonal bipyramidal and ScO₆₊₁ capped octahedral coordination polyhedra. Sc₂(SeO₃)₃·3H₂O contains typical ScO₆ octahedra and is isostructural with its M₂(SeO₃)₃·3H₂O (M=Al, Cr, Fe, Ga) congeners. CsSc₃(SeO₃)₄(HSeO₃)₂·2H₂O contains near-regular ScO₆ octahedra and has essentially the same structure as its indium-containing analogue. All three phases contain the expected pyramidal [SeO₃]^2- selenite groups. Crystal data: Sc₂(SeO₃)₃·3H₂O, M_r=524.85, trigonal, R3c (No. 161), , , , Z=6, R(F)=0.018, wR(F²)=0.036; Sc₂(SeO₃)₃·H₂O, M_r=488.82, orthorhombic, P2₁2₁2₁ (No. 19), , , , , Z=4, R(F)=0.051, wR(F²)=0.086; CsSc₃(SeO₃)₄(HSeO₃)₂·2H₂O, M_r=1067.60, orthorhombic, Pnma (No. 62), , , , , Z=4, R(F)=0.035, wR(F²)=0.070.     

Syntheses, crystal structures, and properties of three new metal selenites Na2Co2(SeO3)3, Na2Co1.67Ni0.33(SeO3)3, and Na2Ni2(SeO3)3

Three new sodium cobalt (nickel) selenite compounds, namely, Na₂Co₂(SeO₃)₃, Na₂Co_1.67Ni_0.33(SeO₃)₃, and Na₂Ni₂(SeO₃)₃ have been hydro-/solvothermally synthesized in the mixed solvents of acetonitrile and water. Single-crystal X-ray diffraction analyses reveal that these isostructural compounds belong to the orthorhombic Cmcm space group and their structures feature three-dimensional open frameworks constructed by the two-dimensional layers of [MSeO₃] pillared by the [SeO₃]²⁻ groups. The two different types of Na⁺ ions reside in the intersecting two-dimensional channels parallel to the a- and c-axes, respectively. Their thermal properties have been investigated via TGA-DSC. The magnetic measurements indicate the existence of the antiferromagnetic interactions in these compounds.     

One-step synthesis of pentavalent triphenylantimony derivatives Ph3Sb(OSiR3)2, Ph3Sb(OCH2CH2)2NH and Ph3Sb(OCH2CH2NMe2)2: X-ray molecular structure of Ph3Sb(OSiMe3)2

Pentavalent bis(triorganosiloxy)triphenylantimony derivatives, Ph₃Sb(OSiR₃)₂ (R = Me, Ph), were synthesized by reaction of triphenylantimony with trimethyl- or triphenylsilanol in the presence of tert-butylhydroperoxide by the mild reaction conditions (0-5 °C, 2 h). The reaction of triphenylantimony with diethanolamine in the presence of tert-butylhydroperoxide gave the cyclic compound Ph₃Sb(OCH₂CH₂)₂NH. The mixture of Ph₃SbO and Ph₃Sb(OCH₂CH₂NMe₂)₂ was obtained by the reaction of triphenylantimony with 2-(N,N-dimethylamino)ethanol in the presence of tert-butylhydroperoxide.     

Syntheses, structures, and properties of Ag4(Mo2O5)(SeO4)2(SeO3) and Ag2(MoO3)3SeO3

Ag₄(Mo₂O₅)(SeO₄)₂(SeO₃) has been synthesized by reacting AgNO₃, MoO₃, and selenic acid under mild hydrothermal conditions. The structure of this compound consists of cis-MoO₂²⁺ molybdenyl units that are bridged to neighboring molybdenyl moieties by selenate anions and by a bridging oxo anion. These dimeric units are joined by selenite anions to yield zigzag one-dimensional chains that extended down the c-axis. Individual chains are polar with the C₂ distortion of the Mo(VI) octahedra aligning on one side of each chain. However, the overall structure is centrosymmetric because neighboring chains have opposite alignment of the C₂ distortion. Upon heating Ag₄(Mo₂O₅)(SeO₄)₂(SeO₃) looses SeO₂ in two distinct steps to yield Ag₂MoO₄. Crystallographic data: (193 K; MoKα, λ=0.71073 Å): orthorhombic, space group Pbcm, a=5.6557(3), b=15.8904(7), c=15.7938(7) Å, V=1419.41(12), Z=4, R(F)=2.72% for 121 parameters with 1829 reflections with I>2σ(I). Ag₂(MoO₃)₃SeO₃ was synthesized by reacting AgNO₃ with MoO₃, SeO₂, and HF under hydrothermal conditions. The structure of Ag₂(MoO₃)₃SeO₃ consists of three crystallographically unique Mo(VI) centers that are in 2+2+2 coordination environments with two long, two intermediate, and two short bonds. These MoO₆ units are connected to form a molybdenyl ribbon that extends along the c-axis. These ribbons are further connected together through tridentate selenite anions to form two-dimensional layers in the [bc] plane. Crystallographic data: (193 K; MoKα, λ=0.71073 Å): monoclinic, space group P2₁/n, a=7.7034(5), b=11.1485(8), c=12.7500(9) Å, β=105.018(1) V=1002.7(2), Z=4, R(F)=3.45% for 164 parameters with 2454 reflections with I>2σ(I). Ag₂(MoO₃)₃SeO₃ decomposes to Ag₂Mo₃O₁₀ on heating above 550 °C.     

EPR study of the NO2+3 radical in irradiated K(UO2)(NO3)3 and K2(UO2)(NO3)4 single crystals

A new radical observed at low temperature in γ-irradiated K₂(UO₂)(NO₃)₄ single crystals has been tentatively assigned to a hitherto unknown oxyanion radical, NO²⁺₃. The assignment and the lack of ¹⁴N hyperfine structure, together with the g factors which are lower than the free-spin value, are discussed in terms of an orbital level scheme.     

Vibrationally excited NO2 from CH3NO2 and 2-C3H7NO2 photodissociation

We observe vibrationally excited NO₂ from photodissociation of CH₃NO₂ and 2-C₃H₇NO₂ by means of laser induced fluorescence. This approximate method shows very large vibrational excitation in all frequencies of NO₂. The result is interpreted as an indirect predissociation.