一种新的测定诺氟沙星的化学发光分析法

基于在碱性条件下,诺氟沙星(NFLX)对鲁米诺-过氧化氢(Luminol-H2O2)化学发光体系的化学发光信号有强烈的抑制作用,建立了一种简单、快速、可连续测定诺氟沙星的流动注射化学发光分析新方法.该方法线性范围为7.0×10-8-1.0×10-6mol/L,检出限(3σ)为1×10-8mol/L,对3.0×10-7m...     

流动注射化学发光分析法测定蒽醌类药物

基于蒽醌类药物在碱性条件下对高碘酸钾-鲁米诺化学发光体系的化学发光信号有强烈的抑制作用这一现象,结合流动注射技术建立了一种直接测定蒽醌类药物的流动注射化学发光分析新方法。该方法测定大黄素的线性范围为1.0×10-8—3.0×10-7g/mL,检出限为2×10-9g/mL;测定大黄酸的线性范围为7.0×10-8—3.0×10-6g/mL,检出限为2×10-8g/mL;测定大黄素甲醚的线性范围为1.0×10-9—5.0×10-8g/mL,检出限为3×10-10g/mL。该方法操作简单快速、灵敏度高,可用于样品中蒽醌类药物含量的准确测定。     

测定双嘧达莫的化学发光新方法

提出了双嘧达莫与高锰酸钾和罗丹明B的化学发光新体系,并发现表面活性剂吐温-80可显著增强该体系的化学发光,据此建立了流动注射化学发光测定双嘧达莫的新方法。该方法选择性好,灵敏度高,线性范围宽,双嘧达莫在5.0×10-8～5.0×10-5g·mL-1范围内与发光信号呈线性关系,检出限1.7×10-8g·mL-1, RSD为1.1%(n=11, c_s=1.0×10-6g·mL-1双嘧达莫浓度)。     

纳米金比色法测定6-巯基嘌呤

在pH 7.0的HAc-NaAc缓冲液溶中,6-巯基嘌呤可以通过Au-S键自组装于金纳米粒子的表面.以Cu2+作为交联剂,Cu2+与6-巯基嘌呤间的配位作用导致金纳米粒子快速发生团聚,金纳米粒子溶液的颜色由红色变为蓝色,最大吸收波长从520nm红移至660nm.660nm和520nm处吸光度的比值(A660/A520)与6-巯基嘌呤的浓度在5.0×10-8-1.0×10-6moL/L范围内存在线性关系.该方法测定6-巯基嘌呤的检出限为1.4×10-8moL/L,相对标准偏差为2.9％(2.0×10-7mol/L 6-巯基嘌呤溶液,n=11).该方法已用于人血清中的6-巯基嘌呤含量的测定.     

Luminol-Cu(Ⅱ)体系流动注射化学发光法测定乙酰半胱氨酸

发现了Luminol-Cu(Ⅱ)-乙酰半胱氨酸化学发光体系,探讨了影响化学发光反应的各个因素,建立了测定乙酰半胱氨酸的流动注射化学发光新方法。该方法的线性范围为7.0×10-10—1.0×10-7g/mL,检出限为2.0×10-11g/mL,相对标准偏差为1.0%(1.0×10-8g/mL,n=11)。该方法已用于药物制剂中乙酰半胱氨酸含量的测定。     

流动注射化学发光法测定L-乳酸铝

发现L-乳酸铝对纳米金-酸性高锰酸钾体系化学发光的增强作用,其增强化学发光强度的能力与高锰酸钾及溶液的介质硫酸浓度、金浓度以及蠕动泵的转速、流动注射化学反应体系的流路设计等因素有关,在此基础上首次建立了测定L-乳酸铝的增强化学发光分析法。测定L-乳酸铝的线性范围为7.0×10-5～1.0×10-2g.mL-1,检出限为1.04×10-6g.mL-1(S/N=3),对8.0×10-4g.mL-1的L-乳酸铝标准溶液进行11次平行测定,相对标准偏差(RSD)为1.48%。该法直接用于L-乳酸铝制备合成反应液以及分离纯化废液中L-乳酸铝的测定,其回收率为95.8%～100.4%,本法与GB/T6987.8-2001法进行了对照,结果令人满意。探讨了该化学发光增强作用是由于L-乳酸铝注入体系后,加速了纳米金与酸性高锰酸钾的反应所致。     

水中铅离子的化学发光分析

基于Pb2+能置换出Co-EDTA络合物中的Co2+和鲁米诺-H2O2-Co2+化学发光体系相偶合,建立了简易、快速测定Pb2+的置换偶合反应流动注射化学发光新方法.在最佳的实验条件下,该方法测Pb2+的线性范围为1.0×10-7-1.0×10-5g/mL,检出限为5×10-8g/mL (3σ),对浓度为1.0×10-...     

酚类物质在鲁米诺-硝酸银-纳米金体系中化学发光行为研究

鲁米诺-硝酸银-纳米金体系有很强的化学发光现象。当向该体系中加入酚类物质,化学发光信号有不同程度的变化。研究发现,酚类物质的—OH可以与纳米金产生相互作用,相互作用的大小与酚类物质所含的—OH数目、位置有关。结合流动注射化学发光法对对苯二酚、邻苯二酚、邻苯三酚进行了测定,检出限分别为4.0×10~(-11),8.0×10~(-10),2.6×10~(-9)g/mL。用加标回收法测定了自来水中的邻苯二酚,回收率在97.5%~105%,相对标准偏差在1.4%~2.5%,结果满意。初步讨论了酚类物质对此体系化学发光强度影响的机理,建立了测定多酚类物质的化学发光分析新方法。     

甲胺磷的流动注射化学发光分析研究

基于甲胺磷对铁氰化钾和鲁米诺在碱性条件下化学发光反应的增强作用,建立了一种甲胺磷的流动注射化学发光(FI-CL)检测方法.甲胺磷浓度在1.0×10-8-1.0×10-5 g/mL范围内与发光强度呈现良好的线性关系,检出限(S/N=3)为3.3×10-9g/mL,测定相对标准偏差(RSD)为2.0%.方法应用于蔬菜中甲胺磷测定,回收率为93.0%-94.4%.文中还研究了化学发光体系的反应机理.     

基于气相沉积等离激元纳米粒子/三维石墨烯-镍泡沫复合结构的高灵敏度表面增强拉曼检测

本文提出一种基于气相沉积银纳米粒子和三维石墨烯-镍泡沫的复合等离激元结构.该结构是利用气相纳米团簇束流技术将高密度的银纳米粒子直接沉积于三维石墨烯-镍泡沫的表面制备而成.与传统银纳米结构相比,复合三维等离激元纳米结构具有"热点"数量多,局域场更强的特点,可作为基于表面增强拉曼技术的高灵敏度化学传感器.拉曼测试实验结果表明,该三维纳米结构在表面增强拉曼检测中可获得灵敏度高,重复性好的探针拉曼信号.通过进一步的理论模拟,发现该三维等离激元结构中增强的拉曼信号主要归因于纳米粒子与纳米粒子之间以及纳米粒子与石墨烯-镍泡沫衬底之间的多重近场耦合效应.     

Chiral perturbation theory for fDS/FD and BBS/BB

The decay constants for D and D_s mesons, denoted f_D and f_DS respectively, are equal in the SU(3)_V limit, as are the hadronic amplitudes for and mixing. The leading SU(3)_V violating contribution to (F_DS/F_D) and to the ration of hadronic matrix elements relevant for and mixing amplitudes are calculated in chiral perturbatiion theory. We discuss the formalism needed to include both meson and anti-meson fields in the heavy quark effective theory.     

Spinor techniques for calculating pp → W±/Z0 + jets

We present techniques which enable one to calculate quickly the amplitudes for many scattering processes in the high-energy limit. As an illustration of the method, these are applied to the diagrams for $\text{p}\text{p}\text{→}\text{V}\text{+ 0, 1}\text{or}\text{2}\text{jets}$, where V = W^± or Z⁰. The form of the results lends itself to immediate numerical evaluation.     

Near-infrared bands of S2: 3Πgi-3Σu+ system

Vibrational and rotational analyses of the near-infrared bands of S₂ lying in the region 7440–8085 Å are reported. They form a new band system involving a ${}^3\text{Π}{}_{\mathrm{gi}}\text{-}{}^3\text{Σ}{}_{\mathrm{u}}{}^{\mathrm{+}}$ transition and arise from the same initial ³Π_gi state of the ³Π_gi-³Δ_ui band system reported earlier. The analyses of the bands of this system due to the isotopic molecules ³²S³⁴S and ³⁴S₂ are also reported.     

Magnetism in nanometer-thick TiOx/Co/TiOx/TiN/Si multilayered structures

Most studies on Co-doped TiO₂ system were focused on thin films grown by MBE-based methods. In this work we report the ferromagnetism of nanometer-thick-layered TiO₂/Co/TiO₂/TiN film grown on Si substrate by conventional magnetron sputtering. For the growth of TiO₂ on silicon, a non-oxide thermally stable material, TiN, was introduced to prevent Ti penetration into the Si substrate. Structural, magnetic, and transport measurements respectively by Raman, SQUID and Hall effect show that our samples are n-type semiconductors and exchange bias effect due to exchange coupling between Co and interfacial CoO. For the rapid vacuum annealed specimen, we found an enhanced loss and a Perminvar-type constricted hysteresis loop, which attributed to pinning of domain walls due to an induced anisotropy by the pair ordering in the metallic alloy of Co-Ti-Si.     

The decay processes Λ8Li → π− + 8Be1 (∼ 17 MeV)

The branching ratio is calculated for _Λ⁸Li decay to the (2⁺) ⁸Be¹ states near 17 MeV, using intermediate coupling wave functions for _Λ⁸Li and for the relevant ⁸Be¹ states. It is pointed out that this ratio is sensitive primarily to a mixing angle ? in the _Λ⁸Li wave function. Within one standard deviation, the data allow two ranges (+0.05 to +0.25 rad and +1.10 to +1.25 rad) for the value of ?. The further requirement that there also be acceptable agreement between the angular distribution expected for the subsequent ${}^8\text{Be}{}^1\text{(? 17}\text{MeV → 2}{}^4\text{He}$ decay and the data, shifts these allowed ranges for ?, to (+0.13 to 0.40) rad and (+0.9 to +1.2) rad. It is predicted that the dominant transition should be to ⁸Be¹ (16.6 MeV), as is observed to be the case, rather than to ⁸Be¹ (16.9 MeV). The interpretation of these values for ? is discussed in some detail and their implications for intermediate coupling shell-model calculations of Λ-hypernuclear wave functions are considered.     

The 5T2g → 5Eg absorption in MgO: Fe2+

At helium temperatures two sharp lines at 9350 and 9510 cm^?1 have been observed for the first tune on the low-energy side of the broad double-peaked absorption corresponding to the ${}^5\text{T}{}_{\mathrm{2g}}\text{→}{}^5\text{E}{}_{\mathrm{g}}$ transition in Fe²⁺ at the octahedral site in MgO. The lower energy line has a half width of 4 cm^?1; Zeeman measurements show that it is of magnetic dipole origin. The Zeeman spectra are consistent with those expected for a pure electronic transition from the (⁵T_2g)T_2g ground state to the ⁵E_g excited state. The second line, with a halfwidth of ~ 35 cm^?1, a vibrational sideband.     

The decay process 11ΛB → π− + 11C

The branching ratios are calculated for ¹¹_ΛB decay to the ¹¹C ground and excited states below 8 MeV for two possible spin values of ¹¹_ΛB. It is found that the decay rate to the ¹¹C^★ state at E^★ = 6.48 MeV is comparable in magnitude to that leading to the ¹¹C ground state if $\text{J(}{}^{11}{}_{\mathrm{\Lambda }}\text{B}\text{) =}\text{5}\text{2}$ is assumed. This result, unlike the branching ratios calculated for the $\text{J(}{}^{11}{}_{\mathrm{\Lambda }}\text{B}\text{) =}\text{7}\text{2}$ case, is in accord with experiment and lends support to the assumption that $\text{J =}\text{5}\text{2}$ holds for ¹¹_ΛB. The necessity of the reinterpretation of some of the so-called ¹³_ΛC events in terms of ${}^{11}{}_{\mathrm{\Lambda }}\text{B}\text{→ π}{}^{\mathrm{?}}\text{+}{}^{11}\text{C}{}^1$ is indicated.     

Electrical property of HfOxNy-HfO2-HfOxNy sandwich-stack films

The effects of HfO_xN_y on the electrical property of HfO_xN_y-HfO₂-HfO_xN_y sandwich-stack (signed as SS) films were investigated. Excellent electrical performances were achieved in SS films, with a high dielectric constant of 16 and a low leakage current of ∼2 × 10⁻⁸ A/cm² at 1 MV/cm. Schottky (SK) emission and Frenkel-Poole (PF) emission are found to be the dominant mechanisms for the current conduction behavior. After a long time stress, the flat-band voltage shift in the SS film is much smaller than that in a pure HfO_xN_y film indicating fewer charge traps existed in the SS film. Based on the experiments, the new SS structure is more favorable for the improvement of electrical performances than a pure HfO_xN_y or HfO₂ structure.     

Electronic and magnetic structures of V-doped zinc blende Zn1-xVxNyO1-y and Zn1-xVxPyO1-y

Electronic and magnetic structures of zinc blende ZnO doped with V impurities are studied by first-principles calculations based on the Korringa-Kohn-Rostoker (KKR) method combined with the coherent potential approximation (CPA).Calculations for the substitution of O by N or P are performed and the magnetic moment is found to be sensitive to the N or P content.Furthermore,the system exhibits a half-metallic band structure accompanied by the broadening of vanadium bands.The mechanism responsible for ferromagnetism is also discussed and the stability of the ferromagnetic state compared with that of the paramagnetic state is systematically investigated by calculating the total energy difference between them by using supercell method.     

Etude par diffraction neutronique des solutions solides K1−xBixF1+2xetRb1−xBixF1+2x

Bragg neutron diffraction studies have been carried out on the fluorite type solid solutions K_1?xBi_xF_1+2x (0.50 ? × ? 0.70) and Rb_1?xBi_xF_1+2x (0.50 ? × ? 0.60). The distribution of the fluorine atoms between normal and interstitial sites is given as a function of substitution rate. A substition mechanism is proposed. Electrical and NMR results on one side and structural data on the other side are correlated. A study of the background as a function of temperature has allowed to determine the static origin of its modulation. By inelastic neutron diffusion, it has been shown that the number of carriers is weak, which involves a high mobility.