2-(2-氨基苯基)苯并噻唑与四苯基卟啉及四苯基锌卟啉的荧光共振能量转移

采用紫外光谱和荧光光谱法研究了四氢呋喃溶液中2-(2-氨基苯基)苯并噻唑(APBT)与四苯基卟啉(TPP)、四苯基锌卟啉(ZnTPP)之间的相互作用。结果表明,APBT可作为能量供体分子分别与能量受体分子TPP或ZnTPP构成荧光共振能量转移(FRET)体系,APBT的作用将使TPP和ZnTPP的荧光增强。在此FRET体系中,APBT与TPP及ZnTPP作用的分子结合比分别为2∶1和3∶1,能量转移效率分别为0.180 3和0.137 5,能量转移临界距离分别为3.76和3.44 nm,供体-受体分子间距离分别为4.31和3.88 nm。     

CdS量子点与曙红Y间的荧光共振能量转移研究

在水溶液中,量子点与有机荧光染料之间可能发生荧光共振能量转移(FRET)。本文以发射波长470nm的Cd S量子点为供体,曙红Y为受体,建立了Cd S量子点-曙红Y的FRET体系,研究了该体系的FRET参数。该体系受体供体数目比为8,猝灭效率为45.6%,增强效率为20.1%;供体-受体间的距离为4.4nm;临界能量转移距离为2.4nm。     

CdTe量子点与罗丹明6G荧光共振能量转移体系的构建及机理研究

以巯基乙酸为修饰剂,水相合成不同尺寸的CdTe量子点(QDs),研究不同发射波长的CdTe QDs与罗丹明6G(R6G)之间的荧光共振能量转移(FRET)规律。结果发现,以发射波长为515nm的CdTe QDs为供体与R6G能量转移效率为58.5%,以R6G为供体与发射波长为605nm的CdTe QDs能量转移效率为49.4%,即在CdTe QDs-R6G的FRET体系中,量子点既可作为供体也可作为受体。在此基础上,构建了CdTe QDs(供体)-R6G(第一受体)-CdTe QDs(第二受体)的三元FRET体系,并研究了其双荧光共振能量转移的机理。     

CdTe量子点-罗丹明6G荧光共振能量转移体系的构建及其应用研究

采用巯基化合物修饰的CdTe量子点构建了量子点(供体)-罗丹明6G(受体)荧光共振能量转移体系, 研究了CdTe量子点与牛血清白蛋白(BSA)的相互作用. 结果表明, CdTe量子点与BSA相互作用后提高了CdTe量子点-罗丹明6G 体系的荧光共振能量转移(FRET)效率, 减小了CdTe量子点和罗丹明6G分子间的距离(r), 证实BSA是通过其色氨酸(Trp)残基与CdTe量子点表面金属发生配位作用而直接结合到量子点表面的.     

基于Ⅰ型核壳量子点的宽光谱响应的高效能量转移体系

针对常规F?rster共振能量转移(FRET)体系中能量转移效率低的问题,合成了可见光吸收的Ⅰ型CIS@Zn S核-壳量子点作为能量供体,近红外方酸(SQ)染料作为能量受体,采用超声自组装的方式首次制备了光谱匹配、间距可调的高效FRET能量转移体系.超快/时间分辨光谱证明了CIS和SQ之间的FRET能量转移机制:CIS*+SQ→CIS+SQ*.荧光猝灭动力学数据显示,CIS@Zn S与SQ之间的能量转移对量子点的尺寸存在依赖性,由CIS@Zn S尺寸增加引起的荧光量子产率和供体-受体间距的增加使得体系的FRET能量转移效率(ηFRET)先增大后减小,并且在壳层反应时间为20min时体系的ηFRET值达到最佳值62.8%.该研究对于开发新型、高效、全谱响应的太阳能电池将具有一定的理论及实际应用价值.     

量子点-罗丹明B比率型荧光探针的制备与性能

本文采用CdSe/Cd_xZn_(1-x)S核/合金壳量子点(QDs)作为荧光共振能量转移体系(FRET)的供体,通过巯基络合作用在其表面修饰一层L-半胱氨酸(Cys)分子,赋予QDs优异的水溶性能,再通过静电相互作用将罗丹明B(RhB)构筑于QDs-Cys表面,获得了一类新型的水溶性FRET体系.采用荧光光谱分析了pH以及供受体浓度比对FRET能量转移效率的影响.研究结果表明,通过静电结合构筑的QDs-Cys-RhB荧光共振能量转移体系对pH和供受体浓度具有敏感的荧光信号响应性能.当pH从10降到7时,FRET体系的荧光共振能量转移效率由49.39%增加到58.99%;当供受体浓度比为3:1时,FRET体系的能量转移效率高达61.09%.由此可见,通过表面络合与静电相互作用构筑的QDs-Cys-RhB荧光共振能量转移体系具有优异的光信号响应性,可以作为一类灵敏、精确的可调式比率型荧光探针,在生物检测、免疫分子等领域中具有广阔的应用前景.     

基于上转换荧光共振能量转移的Hg~(2+)侧流检测模型的设计和应用

本工作利用荧光共振能量转移(FRET)过程,以上转换荧光纳米材料(UCNPs)作为能量供体,以金纳米粒子(AuNPs)作为能量受体,通过适配体识别Hg~(2+),在硝化纤维素膜(NC)上制备侧流检测试纸条。Hg2+的参与会拉近能量供受体距离,引起检测区UCNPs的荧光猝灭。通过检测区的荧光猝灭效率,可判断样品中的Hg~(2+)浓度。该传感器在缓冲溶液中的检测线性范围为0.1~100nmol/L;检出限为0.1nmol/L。本研究成功证实了上转换荧光共振能量转移体系在侧流模型应用的可行性。     

基于I型核壳量子点的宽光谱响应的高效能量转移体系

针对常规Förster共振能量转移(FRET)体系中能量转移效率低的问题, 合成了可见光吸收的I型CIS@ZnS核-壳量子点作为能量供体, 近红外方酸(SQ)染料作为能量受体, 采用超声自组装的方式首次制备了光谱匹配、间距可调的高效FRET能量转移体系. 超快/时间分辨光谱证明了CIS和SQ之间的FRET能量转移机制: CIS*+SQ→CIS+SQ*. 荧光猝灭动力学数据显示, CIS@ZnS与SQ之间的能量转移对量子点的尺寸存在依赖性, 由CIS@ZnS尺寸增加引起的荧光量子产率和供体-受体间距的增加使得体系的FRET能量转移效率(η_FRET)先增大后减小, 并且在壳层反应时间为20 min时体系的η_FRET值达到最佳值62.8%. 该研究对于开发新型、高效、全谱响应的太阳能电池将具有一定的理论及实际应用价值.     

基于2-羟丙基-β-环糊精修饰的CdTe荧光探针定量分析结晶紫及机理探讨

在稳定剂巯基乙酸(TGA)和修饰剂2-羟丙基-β-环糊精(2-Hp-β-CD)存在下,获得的2-Hp-β-CDCdTe量子点具有高的荧光强度、水溶性和光稳定性,以及对结晶紫(CV)的良好包含能力。利用紫外-可见吸收光谱、荧光光谱及TEM图谱,研究了2-Hp-β-CDCdTe量子点与CV的相互作用情况。通过十六烷基三甲基溴化铵(CTAB)作用,显著降低了供体与受体之间的距离,促使量子点与结晶紫发生能量转移,且量子点的荧光光谱与CV的吸收光谱有效重叠,据此建立了量子点与CV的荧光共振能量转移(FRET)体系,并用于CV含量的测定。结果表明,在pH 8.0的Tris-HCl缓冲液中,当存在CTAB时,CV能对2-Hp-β-CDCdTe量子点的荧光峰发生猝灭,且CV浓度在1.0×10~(-7)～1.0×10~(-5) mol/L范围内与量子点的荧光强度变化(ΔF)呈良好线性关系(r~2=0.995 2),检出限为1.74×10~(-8) mol/L,平均回收率为99.0%～106%。     

基于水溶性共轭聚合物分子刷的肿瘤标志物快速检测

以水溶性聚对苯撑乙炔分子刷(PPEB)为传感材料,荧光素标记的多肽为识别探针,设计了一种可实现肿瘤标志物快速、灵敏检测的蛋白质传感器。PPEB的刷状结构带有大量正电荷,与带负电荷的多肽形成静电复合物,使能量供体(PPEB)与受体(荧光素)之间的距离较近,发生高效荧光共振能量转移(FRET)。当多肽探针被前列腺特异性抗原(PSA)识别并切割为更小的寡肽片段时,由于肽段所带电荷量和等电点的变化,其与PPEB之间的静电作用减弱,能量供体和受体之间的距离增大,FRET效率降低。该传感器对PSA的检测可在40min内完成,具有良好的特异性和灵敏度。     

Sc2MgGa2 and Y2MgGa2

Scandium magnesium gallide, Sc₂MgGa₂, and yttrium magnesium gallide, Y₂MgGa₂, were synthesized from the corresponding elements by heating under an argon atmosphere in an induction furnace. These intermetallic compounds crystallize in the tetragonal Mo₂FeB₂‐type structure. All three crystallographically unique atoms occupy special positions and the site symmetries of (Sc/Y, Ga) and Mg are m2m and 4/m, respectively. The coordinations around Sc/Y, Mg and Ga are pentagonal (Sc/Y), tetragonal (Mg) and triangular (Ga) prisms, with four (Mg) or three (Ga) additional capping atoms leading to the coordination numbers [10], [8+4] and [6+3], respectively. The crystal structure of Sc₂MgGa₂ was determined from single‐crystal diffraction intensities and the isostructural Y₂MgGa₂ was identified from powder diffraction data.     

Electrochemical study of (NEt4)2Cl2FeS2MoS2 and (NEt4)2Cl2FeS2MoS2FeCl2

Summary The ability of [MoS₄]^2–, anions to be used as ligands for transition metal ions has been widely demonstrated, especially with Fe²⁺. The present study has been restricted to linear complexes such as (NEt₄)₂ [Cl₂FeS₂MoS₂] and (NEt₄)₂[Cl₂FeS₂MoS₂FeCl₂]. Their electrochemical properties are described: upon electrochemical reduction, these compounds yield MoS₂, as a black precipitate, and an iron complex in solution, assumed to be [SFeCl₂]^2–. The electrochemical reduction goes through two electron transfers, coupled with the breakdown of the molecular skeleton: a DISPl and an ECE mechanism. Depending on the solvent, the following equilibrium may be observed: [Cl₄Fe₂MoS₄]^2–[Cl₂FeMoS₄]^2–+FeCl₂. The equilibrium constant, K_D, was evaluated by differential pulse polarography. K_D is tightly related to the donor number of the solvent.     

The alkali hypophosphites KH2PO2, RbH2PO2 and CsH2PO2

The structures of the hypophosphites KH₂PO₂ (potassium hypophosphite), RbH₂PO₂ (rubidium hypophosphite) and CsH₂PO₂ (caesium hypophosphite) have been determined by single‐crystal X‐ray diffraction. The structures consist of layers of alkali cations and hypophosphite anions, with the latter bridging four cations within the same layer. The Rb and Cs hypophosphites are isomorphous.     

Zur Kenntnis der Dialkalimetalldichalkogenide β-Na2S2, K2S2, α-Rb2S2, β-Rb2S2, K2Se2, Rb2Se2, α-K2Te2, β-K2Te2 und Rb2Te2

On Dialkali Metal Dichalcogenides β-Na₂S₂, K₂S₂, α-Rb₂S₂, β-Rb₂S₂, K₂Se₂, Rb₂Se₂, α-K₂Te₂, β-K₂Te₂ and Rb₂Te₂ The first presentation of pure samples of α- and β-Rb₂S₂, α- and β-K₂Te₂, and Rb₂Te₂ is described. Using single crystals of K₂S₂ and K₂Se₂, received by ammonothermal synthesis, the structure of the Na₂O₂ type and by using single crystals of β-Na₂S₂ and β-K₂Te₂ the Li₂O₂ type structure will be refined. By combined investigations with temperature-dependent Guinier-, neutron diffraction-, thermal analysis, and Raman-spectroscopy the nature of the monotropic phase transition from the Na₂O₂ type to the Li₂O₂ type will be explained by means of the examples α-/β-Na₂S₂ and α-/β-K₂Te₂. A further case of dimorphic condition as well as the monotropic phase transition of α- and β-Rb₂S₂ is presented. The existing areas of the structure fields of the dialkali metal dichalcogenides are limited by the model of the polar covalence.     

Formal [(2+2)+2] and [(2+2)+(2+2)] nonconjugated dienediyne cascade cycloadditions

[reaction: see text] Fluoranthene 2 and heptacycle 3 are easily accessible from the reaction of diyne 1 and norbornadiene (NBD) in the presence of the rhodium catalyst. The unusual [(2+2)+(2+2)] adduct 3 was confirmed by the X-ray crystal structure analysis.     

Crystal Structures of [Bu2Sn(O2PPh2)2], [Ph2Sn(O2PPh2)2], and [PhClSn(O2PPh2)OMe]2. Raman Spectra of [Ph2Sn(O2PPh2)2] and [PhClSn(O2PPh2)OMe]2

[(n‐Bu)₂Sn(O₂PPh₂)₂] ( 1 ), and [Ph₂Sn(O₂PPh₂)₂] ( 2 ) have been synthesized by the reactions of R₂SnCl₂ (R=n‐Bu, Ph) with HO₂PPh₂ in Methanol. From the reaction of Ph₂SnCl₂ with diphenylphosphinic acid a third product [PhClSn(O₂PPh₂)OMe]₂ ( 3 ) could be isolated. X‐ray diffraction studies show 1 to crystallize in the monoclinic space group P2₁/c with a = 1303.7(1) pm, b = 2286.9(2) pm, c = 1063.1(1) pm, β = 94.383(6)°, and Z = 4. 2 crystallizes triclinic in the space group , the cell parameters being a = 1293.2(2) pm, b = 1478.5(4) pm, c = 1507.2(3) pm, α = 98.86(3)°, β = 109.63(2)°, γ = 114.88(2)°, and Z = 2. Both compounds form arrays of eight‐membered rings (SnOPO)₂ linked at the tin atoms to form chains of infinite length. The dimer 3 consists of a like ring, in which the tin atoms are bridged by methoxo groups. It crystallizes triclinic in space group with a = 946.4(1) pm, b = 963.7(1) pm, c = 1174.2(1) pm, α = 82.495(6)°, β = 66.451(6)°, γ = 74.922(6)°, and Z = 1 for the dimer. The Raman spectra of 2 and 3 are given and discussed.     

Die Photoionenspektren von SCl2, S2Cl2 und S2Br2

Photoionization Mass Spectra of SCl₂, S₂Cl₂, and S₂Br₂ Photoionization mass spectra of SCl₂, S₂Cl₂, and S₂Br₂ have been measured. Heats of formation, bond energies, and ionization potentials of fragments have been calculated from appearance potentials.