基于Ru（bpy）3^2＋印刷电极的电致化学发光传感器的研制

利用丝网印刷技术制备了基于Ru(bpy)23 (钌联吡啶)的印刷电极电致化学发光传感器,这种传感器具有制作简单、成本低、重现性好、对草酸盐的响应范围宽、检测限低等优点。详细研究了电极的制作方法以及发光试剂的固定化。在最优条件下,在pH 6.0的0.2 mol.L-1磷酸盐缓冲液中,利用所研制的ECL传感器测定C2O24-,线性响应范围为3.0×10-7~1.0×0-5mol.L-1,检测限为1.2×10-7mol.L-1(S/N=3)。根据同样的原理也可以用来测定其他的成分,如氨基酸,TprA(三丙胺),NAD(烟酰胺腺嘌呤二核苷酸)等物质。同时应该指出的是如果使用丝网印刷机器进行印刷的话,电极的重现性和稳定性还可以进一步提高。     

基于Ru(bpy)_3~(2+)印刷电极的电致化学发光传感器的研制

利用丝网印刷技术制备了基于Ru(bpy)23+(钌联吡啶)的印刷电极电致化学发光传感器,这种传感器具有制作简单、成本低、重现性好、对草酸盐的响应范围宽、检测限低等优点。详细研究了电极的制作方法以及发光试剂的固定化。在最优条件下,在pH 6.0的0.2 mol.L-1磷酸盐缓冲液中,利用所研制的ECL传感器测定C2O24-,线性响应范围为3.0×10-7~1.0×0-5mol.L-1,检测限为1.2×10-7mol.L-1(S/N=3)。根据同样的原理也可以用来测定其他的成分,如氨基酸,TprA(三丙胺),NAD(烟酰胺腺嘌呤二核苷酸)等物质。同时应该指出的是如果使用丝网印刷机器进行印刷的话,电极的重现性和稳定性还可以进一步提高。     

化学发光法测定尿酸

利用尿酸对碱性luminol-H₂O₂-Co2+化学发光体系具有较强的抑制作用,建立了一种测定尿酸的新方法。方法的线性范围为1.0×10-10～7.0×10-6 mol·L-1,检测限(3σ)为1.1×10-11 mol·L-1,RSD 1.9%(n=4,ｃ_s=5.0×10-8 mol·L-1)。该法用于人体血清及尿液中尿酸的测定,结果满意。     

化学发光法测定左氧氟沙星

利用左氧氟沙星对碱性luminol H2 O2 化学发光体系具有强的增敏作用 ,建立了一种测定左氧氟沙星的新方法。方法的线性范围为 5 5 3× 10 - 1 1 ～ 2 2 1× 10 - 8mol·L- 1 ,检测限 (3σ)为 1 38× 10 - 1 1 mol·L- 1 ,RSD为2 5 6 % (n=9)。该法用于胶囊的测定 ,结果满意。     

测定司帕沙星的化学发光分析方法

基于在氢氧化钠介质中,司帕沙星对luminol-H2O2化学发光体系有明显的抑制作用,结合流动注射分析技术,建立了流动注射化学发光法测定司帕沙星药物的新方法.在优化的实验条件下,测定司帕沙星的线性范围是1.0×10-7-1.0×10-5mol·L-1,检出限为1.0×10-8mol·L-1,相对标准偏差（1.0×10-7mol·L-1的司帕沙星,n=11）为1.4％.     

流动注射化学发光法灵敏检测牛血清白蛋白

基于牛血清白蛋白(BSA)在碱性介质中对luminol-H₂O₂体系化学发光的增敏作用,结合流动注射化学发光技术提出了一种快速、 灵敏检测BSA的新方法。在优化条件下,检测BSA的线性范围为2.5×10-9～1.0×10-6 mol·L-1,检出限为5.8×10-10 mol·L-1,样品检测速率达112个·h-1。对1.0×10-7 mol·L-1 BSA溶液重复测定11次,相对标准偏差RSD为0.8%。该方法已成功应用于实际样品牛血清中BSA含量的测定。结合化学发光光谱和紫外可见吸收光谱,对luminol-H₂O₂-BSA体系可能的反应机理进行了探讨。     

吡罗红为底物的辣根过氧化物酶催化荧光反应测定葡萄糖

吡罗红在辣根过氧化物酶催化下可被过氧化氢氧化而使其荧光猝灭。在pH 7.2中性介质中,稳态催化速率由酶和底物浓度决定,催化体系服从Michaelis-Menten方程,用Lineweaver-Burk作图法求得米氏常数、最大反应速度、催化常数分别为2.4×10~(-5)mol·L-1,2.5×10~(-6)mol·L-1s-1,75.8 s-1。在最佳反应条件下,荧光F0/F的猝灭程度与过氧化氢浓度在0-3.6×10~(-7)mol·L-1范围内成线性关系,检测限为6.3×10~(-9)mol·L-1;当与葡萄糖氧化酶联用时,可定量检测葡萄糖,线性关系为0-8.0×10~(-7)mol·L-1,检测限为3.4×10~(-8)mol·L-1。方法用于分析人血清中葡萄糖含量,分析结果与苯酚-4-氨基安替比林法基本一致。     

基于表面增强拉曼光谱的左氧氟沙星检测研究

目前用于检测药物分子的光谱方法主要有荧光光谱法、紫外光谱、红外光谱法等。使用拉曼光谱法检测药物分子的相关信息比较少,表面增强拉曼光谱(SERS)技术具有无损检测、快速灵敏和不受溶剂水的影响等优点。本文开展了基于锌掺杂TiO_2纳米粒子(Zn-TiO_2NPs)作为SERS活性基底的左氧氟沙星(LVFX)药物分子的检测研究。研究结果表明,使用SERS技术对左氧氟沙星进行定性定量分析其检测限可以达到1×10-7 mol·L-1,其定量范围为1×10-31×10-7 mol·L-1。     

EHPG-Tb(Ⅲ)体系荧光法测定稀土铽的研究

采用荧光光谱分析法,探索了N-N’-乙烯-二[2-(2羟基苯基)甘氨酸](EHPG)测定铽离子的最佳条件,建立了稀土铽的分析方法,在室温条件下,pH在7～9,最大激发和发射波长分别为296和547 nm,EHPG浓度为2.5×10-5 mol·L-1,反应3 min后在75 min内测定。结果表明：铽离子的测定范围为1.0×10-8～1.0×10-5 mol·L-1,检出限为1.18×10-9 mol·L-1,在稀土干扰离子存在下,回收率达98%以上,相对标准偏差为3.02％。供试稀土氧化物样品测试值与其含量吻合。     

间接荧光法测定维生素C

实验发现,抗坏血酸在水溶液中能将无荧光的铈(Ⅳ)离子还原成能发射特征荧光的铈(Ⅲ)离子,加入六偏磷酸钠溶液,可使体系的荧光强度大大增强,由此建立了灵敏间接测定抗坏血酸的新方法。用1 cm石英比色池在激发和发射波长分别为303和340 nm处测定其荧光强度;抗坏血酸在1.0×10-7～8.0×10-6 mol·L-1浓度范围内与体系的荧光强度呈良好的线性关系,相关系数为0.999 7,检出限为1.6×10-8 mol·L-1(S/N=3)。     

Magnetic ordering in HoRu2Si2, HoRh2Si2, TbRh2Si2 and TbIr2Si2 by neutron diffraction

Neutron diffraction study of polycrystalline HoRu₂Si₂, HoRh₂Si₂, TbRh₂Si₂, and TbIr₂Si₂ was performed in the temperature range between 4.2 and 300 K. For HoRu₂Si₂ the magnetic spin alignment of a linear transverse wave mode below the Néel temperature 19 K is observed. This static moment wave is propagating along the b-axis with k=(0, 0.2, 0) and is polarized in the c-axis. The root-mean-square and maximum saturation moments per Ho atom are 9.26 and 13.09μ_B, respectively. HoRh₂Si₂, TbRh₂Si₂ an TbIr₂Si₂ are simple collinear antiferromagnets of +-+- type with Néel temperatures of (27±1), (98±2) and (72±3) K, respectively. For TbRh₂Si₂ and TbIr₂Si₂ magnetic moments are localized on RE ions only and are aligned along the tetragonal axis, while for HoRh₂Si₂ they form an angle ø = (28±3)°.     

μ+SR study of LaNi2As2, URh2Si2 and CeRh2Si2

Muon spin relaxation experiments have been carried out in the paramagnetic and magnetically ordered states of URh₂Si₂ and CeRh₂Si₂. As the magnetic structure of these compounds is well known, these measurements can help to characterise their magnetic properties probed by μSR and to understand the μSR results of the heavy fermion compounds of the same crystallographic family. Our measurements show that the muons occupy two different crystallographic sites. The spectra of URh₂Si₂ and CeRh₂Si₂ in the magnetically ordered states are very different, probably reflecting their different magnetic structures. The spectra obtained on CeRh₂Si₂ are similar to the published spectra of the heavy fermion compound CeCu_2.1 Si₂. Muon spin rotation measurements on LaNi₂As₂ indicate that the muon is diffusing at 150 K.     

13C-selective IRMPD of CBr2F2/Cl2 and CCl2F2/Br2 systems

The CO₂ TEA laser irradiation of CBr₂F₂ in the presence of Cl₂ yielded ¹³C-enriched CBrClF₂ and ¹³C-enriched CCl₂F₂ under selected experimental conditions. As the photolysis proceeded, the ¹³C concentration of CBrClF₂ decreased gradually and that of CCl₂F₂ increased up to 90% or higher. These results can be explained by the mechanism involving the secondary ¹³C-selective IRMPD of the primary product CBrClF₂. On the other hand, the carbon-containing product for a CCl₂F₂/Br₂ system was only CBrClF₂; the further IRMPD of which probably regenerated CBrClF₂ in the presence of Br₂. The decomposition probabilities of ¹²C- and ¹³C-containing molecules in both systems were measured as functions of laser line, laser fluence, and reactant pressures.     

Polar optic phonons in Hg2Cl2 and Hg2Br2

Far infrared (30–430 cm^?1) reflectivity measurements of Hg₂Cl₂ and Hg₂Br₂ single crystals have been performed in polarized light. The spectra, which are in agreement with group-theoretical predictions, were analyzed by the oscillator fitting procedure and Kramers-Kronig method. The results are compared with the existing data from other measurements and the large anisotropy of polar modes is briefly discussed. The polarization vectors of all long-wavelength symmetry modes were determined group-theoretically.     

Magnetostriction of SmMn2Ge2 and GdMn2Ge2 intermetallic compounds

Longitudinal and transverse magnetostrictions of polycrystalline samples of intermetallic compounds RMn₂Ge₂ (R=Sm or Gd) are measured in pulsed magnetic fields up to 250 kOe. It is found that linear magnetostrictive strains of about 10^?3 arise in a temperature range in which the magnetic field causes a change in the magnetic state of a manganese magnetic subsystem. The results obtained are described within the model of a two-sublattice ferrimagnet with a negative exchange interaction in the manganese subsystem in terms of a strong dependence of this interaction on interatomic distances.     

Superconductivity in LaPd_2Bi_2 with CaBe_2Ge_2-type structure

正Since the discovery of superconductivity in LaFeAsO_(1-x)F_x,the high-T_c iron-based superconductors have been extensively studied from both experimental and theoretical viewpoints [1-8]. However, the mechanism of the unconventional superconductivity is still to be resolved. To     

Structural,magnetic and neutron diffraction studies on TbFe2-TbAl2, TbCo2-TbAl2 and HoCo2-HoAl2

Both pseudobinary systems exhibit large homogeneous regions of cubic and hexagonal Laves phases. Ordering tendencies on crystallographic sites between Al and the transition metals are observed in the hexagonal type.Electron transfer to the transition metals quenches their moments so that they become nonmagnetic at high Al concentrations. The peculiarities in the mechanism of magnetization which appear in rare earth dialuminides when Al is replaced by a transition metal have been studied in detail at cryogenic temperatures.The first replacement of Al results in a decrease in saturation moment. Neutron diffraction verifies the low ordered rare earth sublattice moments and reveals the ‘lost part’ as a disordered component. Considerable magnetic hardness develops in certain regions of concentration often connected with spontaneous increases in magnetization with field. All available evidence suggests the presence of unusual domain wall effects to be responsible for this effect. High remanences develop in both the hexagonal and in the cubic structures in the intermediate region. The development of disordered magnetic components is connected either with the disorder on crystallographic sites or changes in the free electron concentration.