银纳米粒子修饰银电极法测定酪氨酸

通过NaBH₄还原AgNO₃得到胶体银纳米粒子,制作了以该纳米粒子修饰的银电极。研究了银纳米粒子修饰银电极在电催化中的应用,并对相关机理进行了探讨。该修饰电极对醋酸具有电催化活性,但酪氨酸却对该催化信号有明显的抑制作用,因此建立了用胶体银纳米粒子修饰银电极在NaAc-HAc缓冲溶液中检测酪氨酸的方法,并讨论了最佳工作条件。结果表明：在pH = 5.5时,峰电流与酪氨酸的浓度在1.0×10_-8～1.0×10_-3mol L_-1 范围内呈良好的线性关系,检出限为4.2×10_-9 mol L_-1,线性回归方程为Ip (μA) = 7.64 pC – 15.69 ( R = 99.73% )。用该方法检测氨基酸注射液中酪氨酸的含量,加标回收率在95.2%~107.8%之间。     

银掺杂聚L-酪氨酸修饰电极的制备及对尿酸的测定

利用循环伏安法将银和L-酪氨酸聚合修饰在玻碳电极表面,制成银掺杂聚L-酪氨酸(Ag-PLT/GCE)修饰电极,研究了尿酸在该电极上的电化学行为,建立了循环伏安法测定尿酸的新方法。在pH=3.0的磷酸盐缓冲溶液中,扫描速率为100mV/s时,尿酸在该修饰电极上产生一氧化峰,Epa=0.637V(vs.Ag/AgCl)。用循环伏安法进行测定时,峰电流与尿酸浓度在8.0×10-7～1.0×10-5mol/L和1.0×10-5～1.0×10-4mol/L范围内呈良好的线性关系,检出限为3.0×10-7mol/L。方法用于尿样中尿酸的测定,结果满意。     

应用单壁碳纳米管修饰纳米碳纤维电极同时测定多巴胺和抗坏血酸

采用滴涂法制备了单壁碳纳米管修饰的纳米碳纤维电极,研究了多巴胺(DA)、抗坏血酸(AA)及其混合溶液在修饰前后电极上的电化学行为。在20 mmol/L Tris-HCl(pH 7.4)缓冲溶液中,修饰电极对DA和AA具有很好的电催化作用。采用差示脉冲伏安法对DA与AA混合溶液氧化峰电流与浓度的关系进行定量分析,DA和AA的氧化峰电流在1.0×10-7~5.0×10-5mol/L和1.0×10-5~1.0×10-3mol/L范围内与浓度呈线性关系,其线性回归方程及相关系数分别为Ip=0.0012c+4×10-9,r=0.9907;Ip=10-5c+7×10-10,r=0.9974,两种物质的检测限分别达到8.0×10-9mol/L和2×10-6mol/L。     

纳米银粒子修饰电极法测定血红蛋白

报道了一种利用纳米材料修饰电极检测血红蛋白的新方法。制作了以纳米银粒子修饰的银电极,并研究了血红蛋白在该修饰电极上的直接电化学行为。实验结果表明,血红蛋白在该修饰电极上具有良好的电流响应。在2.0×10-7~1.0×10-5mol/L浓度范围内,血红蛋白的氧化峰电流与其浓度呈良好线性关系;检出限为7.4×10-8mol/L。研究了该修饰电极对血红蛋白的催化机理,利用该电极所建立的方法实现了对血红蛋白的分析测定。     

银掺杂聚L-天冬氨酸修饰电极的制备及对多巴胺的测定

利用循环伏安法将银与L-天冬氨酸聚合修饰在玻碳电极表面,制成银掺杂聚L-天冬氨酸修饰电极,研究了多巴胺在此电极上的电化学行为,建立了循环伏安法测定多巴胺的新方法.在磷酸盐缓冲溶液(PBS, pH 7.0)中,扫描速率为50 mV/s时,多巴胺在修饰电极上产生一对氧化还原峰,Epa=0.191 V,Epc=0.161 V.用循环伏安法进行测定时,峰电流与多巴胺浓度分别在3.0×10-7 ～1.0×10-5 mol/L和1.0×10-5 ～5.0×10-4 mol/L内呈良好的线性关系; 检出限为5.0×10-8 mol/L.用于药物和尿样中多巴胺的测定,结果满意.     

线状纳米金修饰碳纤维超微电极检测芦荟大黄素

该文建立了芦荟大黄素(AE)的电化学检测方法。通过柠檬酸三钠还原氯金酸制备线状纳米金,采用一步恒电位沉积方法将线状纳米金沉积在碳纤维超微电极(CFME)表面,考察了电极修饰前后对AE的电催化性能,得到最佳修饰时间为12 min。结果表明,线状纳米金修饰碳纤维电极(LGN/CFME)的氧化峰电流与AE浓度在2.0×10-6~1.0×10-4 mol/L范围内呈良好线性关系,线性方程为Ip(nA)=0.318 1C(μmol/L)+25.01,r2=0.965 3,检出限(S/N=3)为6.19×10-7 mol/L,说明此方法可用于芦荟汁中AE的定量检测。     

碳纳米管/纳米金修饰金电极上柔红霉素电化学行为的研究

将碳纳米管与纳米金结合修饰在金电极上制成修饰电极,并用于柔红霉素(DNR)的电化学行为研究和检测.在4.4 mmol/L磷酸盐缓冲溶液(pH=5.81)中,DNR在碳纳米管-纳米金/Au电极上有一对灵敏的氧化还原峰.还原峰电流与DNR的浓度在3.2×10-8～1.0×10-6mol/L和1.0× 10-6～2.2× 1...     

直接电沉积金纳米粒子修饰氧化铟锡电极测定亚硝酸根

以电化学沉积法一步制得了金纳米粒子(GNP)修饰氧化铟锡(ITO)电极,采用紫外、扫描电镜及循环伏安法对GNP/ITO修饰电极进行了表征。结果表明,金纳米粒子在ITO电极表面呈球形,分布均匀无团聚,粒径约30 nm。该修饰电极具有良好的电化学性能,在pH 2.2的Na2HPO4-柠檬酸缓冲溶液中其氧化峰电流与NO2-的浓度呈良好的线性关系,线性范围为5×10-6~5.5×10-4mol/L,线性回归方程为:i(μA)=1.07 136C(mmol/L),相关系数r=0.9969;检出限可达1.0×10-6mol/L。该修饰电极用于废水中NO2-的测定,结果令人满意。     

介孔炭/纳米金修饰玻碳电极的制备及其应用研究

制备了介孔炭/纳米金修饰玻碳电极,并对对苯二酚(HQ)在该修饰电极上的电化学行为进行了研究。与HQ在纯介孔炭材料修饰玻碳电极上的电化学响应相比,HQ在该修饰电极上的氧化峰和还原峰电流均大大增加,表明纳米金与介孔炭复合后对HQ具有良好的催化作用。HQ在该修饰电极上经过富集后,峰电流明显增大。采用循环伏安法对HQ电化学行为进行研究,结果表明,HQ在3.0×10-8~1.0×10-6mol/L和1.0×10-6~1.0×10-4mol/L浓度范围内与峰电流呈良好的线性关系,据此建立了检测HQ的电化学分析方法。该方法的相对标准偏差为0.69%,检出限(S/N=3)为1.0×10-8mol/L,具有较高的稳定性和灵敏度。     

基于纳米二氧化锆与铂微粒复合修饰玻碳电极的甲醛传感器研究

采用循环伏安法在玻碳电极表面依次电沉积纳米二氧化锆和铂微粒,制备了一种检测甲醛的新型电化学传感器。用电镜扫描对该修饰电极表面进行了表征,循环伏安法和线性扫描伏安法研究了甲醛在该修饰电极上的电催化氧化作用,优化了实验参数。结果表明,该修饰电极对甲醛有很好的电催化氧化作用,在0.1 mol/L H2SO4溶液中,甲醛的氧化峰电流与其浓度在1.0×10-6~5.0×10-3mol/L范围内呈良好线性关系,回归方程为Ip(μA)=79.95+2.005×105c(mol/L),相关系数r=0.999 3,检出限为5.0×10-7mol/L。     

The first measured Ag I, Ag II and Ag III Stark broadening parameters

The Stark widths (W) and shifts (d) of two neutral (520.908 and 546.550 nm), eleven singly (211.382, 224.643, 224.874, 232.029, 232.468, 233.140, 241.141, 241.323, 243.781, 244.793 and 276.754 nm) and three doubly (216.189, 231.004 and 239.569 nm) ionized silver (Ag I, Ag II and Ag III, respectively) spectral lines have been measured in nitrogen plasma at about 18,000 K electron temperature and electron density ranged between 0.65 × 10²³ and 1.15 × 10²³ m^− 3. They are the first measured W and d values while those of the Ag II and Ag III lines are the first published data in these spectra. The modified version of the linear, low-pressure, pulsed arc was used as a plasma source operated in nitrogen with silver atoms, as impurities, evaporated from silver cylindrical plates located in the homogeneous part of the discharge. No theoretical predictions exist for W and d values of above mentioned spectral lines. Besides, we have checked the transition probability ratio of two investigated Ag I lines. An agreement with theoretical predictions was found.     

Ag nanoparticles from the mechanochemical decomposition of Ag oxalate

The present work focuses on the chemical reactivity of Ag oxalate powders under mechanical processing conditions. The powders were submitted to mechanical loads in the presence of an aqueous solution containing a polymeric surfactant. A gradual decrease of the total mass of powders was observed, ascribable to the occurrence of a decomposition process. X-ray diffraction and UV-vis spectrophotometric analyses indicated that the Ag oxalate decomposes into metallic Ag and gaseous carbon dioxide. Transmission electron microscopy showed that metallic Ag exists in the form of particles with average size of about 5 nm. The formation of nanometer-sized Ag particles can be related to the plastic deformation and attrition processes taking place at the points of contacts between neighboring particles during the mechanical loading at collision.     

Disc-Like Silver Nanocluster Ag93 Built with Bicapped Hexagonal Prismatic Ag15 and Ino Decahedral Ag13 Units

The reduction of alkynyl-silver and phosphine-silver precursors with a weak reducing reagent Ph₂SiH₂ led to the formation of a novel silver nanocluster [Ag₉₃(PPh₃)₆(C≡CR)₅₀]³⁺ (R=4-CH₃OC₆H₄), which is the largest structurally characterized cluster of clusters. This disc-shaped cluster has a Ag₆₉ kernel consisting of a bicapped hexagonal prismatic Ag₁₅ unit wrapped by six Ino decahedra through edge-sharing. This is the first time that Ino decahedra are used as a building block to assemble a cluster of clusters. Moreover, the central silver atom has a coordination number of 14, which is the highest in metal nanoclusters. This work provides a diverse metal packing pattern in metal nanoclusters, which is helpful for understanding metal cluster assembling mechanisms.     

Real and Hypothetical Intermediate-Valence Ag(II)/Ag(III) and Ag(II)/Ag(I) Fluoride Systems as Potential Superconductors

With the aim of gauging their potential as conducting or superconducting materials, we examine the crystal structures and magnetic properties of the roughly one hundred binary, ternary, and quaternary Ag(II) and Ag(III) fluorides in the solid state reported up to date. The Ag(II) cation appears in these species usually in a distorted octahedral environment, either in an [AgF](+) infinite chain or as [AgF(2)] sheets. Sometimes one finds discrete square-planar [AgF(4)](2-) ions. The Ag(III) cation occurs usually in the form of isolated square-planar [AgF(4)](-) ions. Systems containing Ag(III) (d(8)) centers are typically diamagnetic. On the other hand, the rich spectrum of Ag(II) (d(9)) environments in binary and ternary fluorides leads to most diverse magnetic properties, ranging from paramagnetism, through temperature-independent paramagnetism (characteristic for half-filled band and metallic behavior) and antiferromagnetism, to weak ferromagnetism. Ag(II) and Ag(III) have the same d-electron count as Cu(II) (d(9)) and Cu(III) (d(8)), respectively. F(-) and O(2-) ions are isoelectronic, closed-shell (s(2)p(6)) species; both are weak-field ligands. Led by these similarities, and by some experimental evidence, we examine analogies between the superconducting cuprates (Cu(II)/Cu(III)-O(2-) and Cu(II)/Cu(I)-O(2-) systems) and the formally mixed-valence Ag(II)/Ag(III)-F(-) and Ag(II)/Ag(I)-F(-) phases. For this purpose we perform electronic-structure computations for a number of structurally characterized binary and ternary Ag(I), Ag(II), and Ag(III) fluorides and compare the results with similar calculations for oxocuprate superconductors. Electronic levels in the vicinity of the Fermi level (x(2)-y(2) or z(2)) have usually strongly mixed Ag(d)/F(p) character and are Ag-F antibonding, thus providing the potential of efficient vibronic coupling (typical for d(9) systems with substantially covalent bonds). According to our computations this is the result not only of a coincidence in orbital energies; surprisingly the Ag-F bonding is substantially covalent in Ag(II) and Ag(III) fluorides. The electron density of state at the Fermi level (DOS(F)) for silver fluoride materials and frequencies of the metal-ligand stretching modes have values close to those for copper oxides. The above features suggest that properly hole- or electron-doped Ag(II) fluorides might be good BCS-type superconductors. We analyze a comproportionation/disproportionation equilibrium in the hole-doped Ag(II) fluorides, and the possible appearance of holes in the F(p) band. It seems that there is a chance of generating an Ag(III)-F(-)/Ag(II)-F(0) "ionic/covalent" curve crossing in the hole-doped Ag(II)-F(-) fluorides, significantly increasing vibronic coupling.     

Structural variation of silver clusters from Ag13 to Ag160

The structures of silver clusters from Ag(121) to Ag(160) were optimized with a modified dynamic lattice searching (DLS) method, named as DLS with constructed core (DLSc). The interaction among silver atoms is modeled by the Gupta potential. Structural characteristic of silver clusters with the growth of cluster size is investigated with the newly optimized structures and our previous results from Ag(13) to Ag(120). A set of amorphous structures was obtained in the size range of 13-48, together with several ordered structures. The putative stable motif is an icosahedron from Ag(49) to Ag(61) and then changes to a decahedron in the size range of 62-160. Some of the results are consistent with experiments. Furthermore, it was also found that, for clusters with decahedral motif, the stable structure is a result of the competition among the different Marks decahedral motifs. On the other hand, different from the Lennard-Jones cluster, there are some silver clusters with the face-centered cubic (fcc) motif in the size range of 13-160. But the fcc motif can only be obtained for some specific sizes.     

Migration of Ag in low-temperature Ag2S from first principles

Using the density-functional theory combined with the nudged elastic band method, we have calculated migration pathways and estimated the activation energy barriers for the diffusion of Ag ions in low-temperature Ag2S. The activation energy barriers for four essential migrations for an Ag ion, namely, from a tetrahedral (T) site to an adjacent T vacancy (VT), from an octahedral (O) site to an adjacent O vacancy (VO), from T to VO, and from O to VT, are estimated as 0.461, 0.668, 0.212, and 0.318 eV, respectively, which are comparable to experimental values. This means that diffusions of Ag ions between nonequivalent sites are preferable to those between equivalent sites, and that direct T-VT and O-VO diffusions are less likely to occur than indirect T-VO-T and O-VT-O diffusions. These diffusion behaviors between nonequivalent sites have also been supported by ab initio molecular dynamics simulations, in which the diffusion pathways are directly observed.     

Ligand and counterion control of Ag(I) architectures: assembly of a {Ag8} ring cluster mediated by hydrophobic and Ag...Ag interactions

A strategy combining ligand design and counterion variation has been used to investigate the assembly of silver(I) complexes. As a result, dinuclear, octanuclear, and polymeric silver(I) species have been synthesized by complexation of the rigid aliphatic amino ligands cis-3,5-diamino-trans-hydroxycyclohexane (DAHC), cis-3,5-diamino-trans-methoxycyclohexane (DAMC), and cis-3,5-diamino-trans-tert-butyldimethylsilylanyloxycyclohexane (DATC) with silver(I) triflate, nitrate, and perchlorate. The compositions of these aggregates, established by X-ray crystallography and elemental analysis, are [{Ag(DAHC)}2](CF3SO3)2 (1), [{Ag(DAMC)}2](CF3SO3)2 (2), [{Ag(DAMC)}2](NO3)2 (3), [{Ag(DATC)}6{Ag(DAHC)}2](NO3)8 (4), and [{Ag(DATC}n](NO3)n (5), where the DAHC present in 4 is formed by in situ hydrolysis of the acid labile silyl ether group. The type of aggregate formed depends both upon the noncoordinating O-substituent of the ligand and the (also noncoordinating) counterion, with the normal preference of the ligand topology for forming Ag2L2 structures being broken by introduction of the bulky, lipophilic O-tert-butyldimethylsilyl (TBDMS) group. Of particular note is the octanuclear silver ring structure 4, which is isolated only when both the O-TBDMS group and the nitrate counteranion are present and is formed from four Ag2L2 dimers connected by Ag...Ag and hydrogen-bonding interactions. Diffusion rate measurement of this {Ag8} complex by 1H NMR (DOSY) indicates dissociation in CD3OD and CD3CN, showing that this supramolecular ring structure is formed upon crystallization, and establishing a qualitative limit to the strength of Ag...Ag interactions in solution. When solutions of the {Ag8} cluster in methanol are kept for several days though, a new UV-vis absorption is observed at around 430 nm, consistent with the formation of silver nanoparticles.     

Cross-Coupling through Ag(I)/Ag(III) Redox Manifold

In ample variety of transformations, the presence of silver as an additive or co-catalyst is believed to be innocuous for the efficiency of the operating metal catalyst. Even though Ag additives are required often as coupling partners, oxidants or halide scavengers, its role as a catalytically competent species is widely neglected in cross-coupling reactions. Most likely, this is due to the erroneously assumed incapacity of Ag to undergo 2e⁻ redox steps. Definite proof is herein provided for the required elementary steps to accomplish the oxidative trifluoromethylation of arenes through Ag^I/Ag^III redox catalysis (i. e. CEL coupling), namely: i) easy Ag^I/Ag^III 2e⁻ oxidation mediated by air; ii) bpy/phen ligation to Ag^III; iii) boron-to-Ag^III aryl transfer; and iv) ulterior reductive elimination of benzotrifluorides from an [aryl-Ag^III-CF₃] fragment. More precisely, an ultimate entry and full characterization of organosilver(III) compounds [K]⁺[Ag^III(CF₃)₄]⁻ ( K-1 ), [(bpy)Ag^III(CF₃)₃] ( 2 ) and [(phen)Ag^III(CF₃)₃] ( 3 ), is described. The utility of 3 in cross-coupling has been showcased unambiguously, and a large variety of arylboron compounds was trifluoromethylated via [Ag^III(aryl)(CF₃)₃]⁻ intermediates. This work breaks with old stereotypes and misconceptions regarding the inability of Ag to undergo cross-coupling by itself.     

Phase equilibria in the Ag2Te-ZnTe and Ag2Te-Zn systems

The state diagrams (T-x) of the systems Ag₂Te-ZnTe(I) and Ag₂Te-Zn(II) are offered on the ground of data obtained by differential thermal analysis, X-ray phase analysis, microstructural analysis and measurements of the density and the microhardness of samples synthesized. The systems studied are quasibinary sections of the ternary system Ag-Zn-Te. System I is characterized by two eutectic and three eutectoidal non-variant equilibria as well as by an intermediate compound Ag₂ZnTe₂, which melts congruently at 880°C. The latter exists in the range from 120 to 880°C in two polymorphic modifications (T_ʅ→β=515°C). System II is characterized by one eutectic, two eutectoidal and one peritectic nonvariant equilibria, boundary solid solutions on the ground of Ag₂Te and Zn and one intermediate phase of the composition Ag₄Zn₃Te₂, which melts congruently at 880°C.