5-甲氧基色醇-酸性高锰酸钾-甲醛化学发光体系研究与应用

在甲醛的存在下 ,5 -甲氧基色醇 (5 - ML)与高锰酸钾在高氯酸介质中发生化学反应 ,能产生很强的化学发光。本文据此采用流动注射技术研究其发光行为 ,对影响化学发光强度的实验因素进行优化 ,建立了快速灵敏测定 5 - ML的化学发光新方法 ,测定方法的线性范围为 2 .0× 10 -8mol/ L— 4 .0× 10 -5mol/ L,检出限为 7.9× 10 -9mol/ L(S/ N=3) ,相对标准偏差为 2 .4 % (5 .7× 10 -7mol/ L5 - ML;n=10 )。该方法应用于脑脊液样品中 5 - ML含量测定 ,回收率达到 86 .0 %— 97.2 %。文中还对体系的化学发光反应机理进行探讨     

高效液相色谱法测定2-对甲氧基苯基-4-苯基-1,5-苯并硫氮杂-α-(丁二酰亚胺基)-β-内酰胺

应用高效液相色谱外标定量法对 2 -对甲氧基苯基 - 4 -苯基 - 1,5 -苯并硫氮杂 艹卓 -α- (丁二酰亚胺基 ) -β-内酰胺进行了测定。采用 Hypersil- ODS2 ( 4 .6mm× 2 5 0 mm,5 μm)柱 ,乙腈与水按 70∶ 30 ( V/ V)组成流动相 ,测定波长为 2 4 2 nm,该方法线性范围为 0— 0 .1mg/ m L ,回归方程 A=1.91× 10 8C- 3.82× 10 5,相关系数 r=0 .9994 ,相对标准偏差为 0 .72 %,检出限为 0 .0 5μg/ m L,平均回收率在 98.4 %— 10 1.8%之间。该法重现性好、灵敏度高、简单、快速。     

7-(苯并噻唑-2-偶氮)-8-羟基喹啉-5-磺酸与镉显色反应的研究和应用

在 p H4 .8的邻苯二甲酸氢钾 - Na OH介质中 ,非离子表面活性剂 Tween- 80存在下 ,7- (苯并噻唑 - 2 -偶氮 ) - 8-羟基喹啉 - 5 -磺酸 (BTAQS)与镉形成 2∶ 1的紫红色配合物 ,其最大吸收波长 λmax=5 6 0 nm,表观摩尔吸光系数为 8.71× 10 4L· mol-1·cm-1,镉含量在 0— 6 μg/ 10 m L范围内服从比耳定律。用于矿样中镉的测定 ,相对误差小于 3% ,相对标准偏差小于 2 .5 % (n=5 )。     

荧光光度法测定胰腺肿瘤细胞膜上的潘生丁

测定了胰腺肿瘤细胞膜上的潘生丁在乙腈 -水溶液中的荧光光谱和强度 ,并推算出胰腺肿瘤细胞膜上核苷载体的数量。潘生丁的浓度与其荧光强度在 1.0× 10 -12 — 5 .0× 10 -5mol/ L范围内呈线性关系 ,检出限为 2 .8× 10 -13 mol/ L(1.4× 10 -4ng/ m L) ,相对标准偏差为 2 .7%。     

高效液相色谱法测定2-苯基-4-对甲苯基-1,5-苯并硫氮杂-α-(丁二酰亚胺基)-β-内酰胺

本文采用 Hypersil- ODS2 (4 .6mm× 2 5 0 mm,5μm)色谱柱 ,乙腈 -水 (70∶ 30 )流动相 ,2 4 2 nm测定波长 ,建立了测定 2 -苯基 4 -对甲苯基 - 1,5 -苯并硫氮杂 艹卓 -α- (丁二酰亚胺基 ) -β-内酰胺高效液相色谱法。该法线性范围为 0— 0 .1mg/ m L,回归方程 A=2 .11× 10 8C- 3.10× 10 5,相关系数 r=0 .9995 ,相对标准偏差为0 .2 4 % (C=0 .0 6mg/ m L,n=5 ) ,检出限为 0 .0 5 μg/ m L。平均回收率在 97.1%— 10 2 .4 %之间。该法重现性好、灵敏度高、简单、快速、准确     

盐酸川芎嗪的荧光光谱研究及应用

在 p H6— 10的水溶液中 ,盐酸川芎嗪产生稳定的荧光。最佳激发波长与发射波长分别为 2 95nm和335nm,当盐酸川芎嗪浓度为 5.0× 10 -6— 5.0× 10 -5mol/ L时 ,荧光强度与浓度有良好的线性关系。据此建立了荧光光度法直接测定盐酸川芎嗪注射液中盐酸川芎嗪含量的方法 ,该方法的相对标准偏差为3.51% ,检出下限为 1.0× 10 -6mol/ L。     

光泽精化学发光体系的研究与应用

对光泽精化学发光体系的动力学性质、荧光光谱、化学发光光谱及化学发光机理进行研究和探讨。详细研究了光泽精 - H2 O2 - Co( )流动注射化学发光体系的最佳分析条件。结果表明 ,当光泽精 (L c)为 2 .5×10 - 5mol/L、H2 O2 为 0 .5 mol/L、Na OH为 0 .4 mol/L、CTMAB为 2 .0× 10 - 5mol/L时 ,测定 Co( )的校准曲线线性范围为 0 .0 5— 2 0 0μg/m L ,检出限为 0 .0 1μg/m L。对 10μg/m L Co( )连续测定 7次 ,相对标准偏差为 1.7%。     

新显色剂四(4-甲氧基-4-磺酸基苯基)卟啉与Fe~(3+)的高灵敏反应的研究与应用

本文提出以四 (4 -甲氧基 - 4 -磺酸基苯基 )卟啉 (p- OCH3TPPS4 )为显色剂 ,在 p H=3.5— 5 .5的条件下测定痕量铁的新体系 ,络合物最大吸收波长为 4 4 6nm,表观摩尔吸收系数ε=2 .0× 10 4 L· mol-1· cm-1,Fe3+ 在 0— 10 μg/ 2 5 m L 范围内符合比耳定律 ,应用本法测定花生仁皮中铁 ,回收率可达 95 .0 %—10 8.4 %     

显色剂1-(2-苯并噻唑)-3-(5,7-二溴-8-喹啉)-三氮烯的合成及与钴的显色反应

合成了新显色剂 1- (2 -苯并噻唑 ) - 3- (5 ,7-二溴 - 8-喹啉 ) -三氮烯 (BTDBQT) ,并研究了在阳离子表面活性剂存在下与钴的显色反应。在 p H9.5— 10 .5的硼酸盐缓冲介质中 ,钴与该试剂形成 1∶ 2的蓝色铬合物 ,其最大吸收波长在 6 42 nm处 ,表观摩尔吸光系数为 1.0 5× 10 5L· mol-1·cm-1,钴 ( )的浓度在0— 2 4 0 μg/ L范围内符合比耳定律。显色反应具有良好的选择性 ,常见离子除铜、镍外 ,基本不干扰测定。已应用于维生素 B12 和水系沉积物中微量钴的测定     

meso-四(4-甲氧基苯基)卟啉分光光度法测定痕量铅的研究

研究了在 p H12和 Tween- 80存在下非水溶性试剂 meso-四 (4 -甲氧基苯基 )卟啉与铅的络合反应条件 ,形成的络合物的最大吸收波长为 4 6 7nm,组成摩尔比为 1∶ 1。铅含量在 0 .1— 8μg/ 10 m L范围内有较好的线性关系 ,表观摩尔吸光系数为 1.12× 10 5L· mol-1· cm-1。本方法应用于环境水样中痕量铅的测定 ,结果令人满意     

Speckle characteristics of a broad-area VCSEL in the incoherent emission regime

We present a technique to reduce the speckle contrast of a NIR broad-area VCSEL based on the spatially incoherent emission regime that can be obtained when using the proper driving conditions. We evaluate the efficiency of this technique to reduce the speckle contrast by comparing it with the speckle characteristics in multimode emission under cw operation. Depending on the illumination setup, the incoherent emission regime can lead to a strongly reduced speckle contrast down to 1.3%. This is in agreement with estimates of the expected speckle contrast reduction when three contrast reducing effects are taken into account. These low contrast values make the investigated sources attractive for several applications that suffer from speckle noise.     

Structural characterization of ultrathin Cr and Sc films for soft X-ray mirrors

The structure of multilayers of ultrathin scandium (Sc) and chromium (Cr) films has been characterized by means of transmission electron microscopy (TEM). Face centered cubic Sc was found both in magnetron sputtered thin Sc layers on Si(0 0 1) and in Cr/Sc multilayers for soft X-ray mirrors. The single Sc and Cr layers are polycrystalline with randomly oriented grains, while Sc and Cr within the Cr/Sc multilayer show a strong [0 0 1] texture in the deposition direction. From high-resolution images the orientation-relationship at the Cr/Sc interfaces could be deduced as: Sc_[110]//Cr_[100] and Sc_[010]//Cr_[110], which was confirmed by image simulations.     

Optical transmission through an interface between subwavelength slits

This paper studies optical transmission through an interface between two slits with different widths in a sheet composed of an ideal conductor. Such a structure is of potential use in fabricating optical diode and may be the simplest one compared to other designs. Our calculations show that there is a critical wavelength. When the light wavelength is below the critical wavelength, the transmissivity is unidirectional. The expression of the stable transmissivity as a function of the ratio of the widths of the two slits was obtained analytically. Particularly, at the critical wavelength, the transmissivities are zero. This phenomenon has great potential for application in the manufacture of wavelength blockers.     

Grain boundary potential and charge density at grain boundaries of chemically prepared thin silver sulfide films

The grain boundary potential and interface state charge density at the grain boundaries of silver sulfide (Ag₂S) thin films prepared by chemical conversion of cadmium sulfide (CdS) films have been determined from the dc resistance of the material and are found to be sensitive to annealing. A reduction in the grain boundary potential and the grain boundary charge density of the film has been noticed when the source CdS film is annealed at different temperatures prior to chemical conversion. The variation in the grain boundary charge density of the grown Ag₂S film with source annealing temperature has been found to be similar to that of thin cadmium sulfide film, reported earlier. An additional low temperature heat treatment of the sample results in an enhancement in the charge density at the grain boundaries. The change in the silver vacancy and/or oxygen and sulfur content of the films as revealed from the energy dispersive spectra of the films suggests possible role of film composition on the grain boundary charge density.     

三螺旋DNA分子Poly(dT)·Poly(dA)·Poly(dT)碱基振动模式

利用晶格动力学方法计算了三螺旋 DNA分子 poly(d T)· poly(d A)· poly(d T)碱基振动模式 ,并根据势能分布矩阵对碱基振动模式进行了指定。计算的模式频率同拉曼光谱实验相符合     

Effect of Ir(pq)2acac doping on CBP in phosphorescence organic light-emitting diodes

Doping is one of the most powerful methods amongst the various performance improvement ways. Doping affects the energy levels of the host layer by the energy level of the dopant. This allows the energy bandgap to be adjusted to a desired level and thus generates light corresponding to that energy level. Alternatively, it can act as an energy barrier between the interfaces to change the flow of carriers. In this study, the voltage dependences of undoped and doped devices were observed. Bis(2-phenylquinoline) iridium(III) (acetylacetonate) (Ir(pq)₂acac) was doped in 4,4′-N, N′-dicarbazole-biphenyl (CBP) as the emission layer. The light intensity changes with the doping concentration, and the efficiency was also studied. When a high voltage was applied, the effect of triplet-triplet annihilation (TTA) adversely affected the electron-hole recombination. We analyzed the optimal operating conditions and the effect of doping concentration on OLEDs.     

Belle实验观测到新类粲偶素结构

利用在Υ(nS)(n=1,2,4,5)共振态及其附近采集的大量数据,Belle实验测量了末态中含两个矢量粒子的双光子过程γγ→J/ψ和ωJ/ψ.在这两个过程中,发现了两个窄共振结构X(4350)和X(3915).这两个新结构的性质目前尚不清楚,可能是普通粲偶素粒子,也可能是含一对粲夸克和一对轻夸克的四夸克态,或含一对粲夸克和一个激发胶子的混杂态,或是由其他未知的动力学原因造成的奇特结构.Belle同时发现在γγ→J/ψ过程中,不存在显著的Y(4140)的信号,实验结果与将Y(4140)解释为四夸克态的部分理论预期有较大差异.     

XYZ particles at Belle

In this paper, I review recent progress in the study of the XYZ particles at Belle. I only focus on studies with charmonium and one or more light mesons in the final states. This covers the X(3872), X(3915),Y(4140), X(4350), and the charged Z states.     

Effect of swift heavy ion irradiation on photoluminescence properties of ZnO/PMMA nanocomposite films

We report a study on the SHI induced modifications on structural and optical properties of ZnO/PMMA nanocomposite films. The ZnO nanoparticles were synthesized by the chemical route using 2-mercaptoethanol as a capping agent. The structure of ZnO nanoparticles was confirmed by XRD, SEM and TEM. These ZnO nanoparticles were dispersed in the PMMA matrix to form ZnO/PMMA nanocomposite films by the solution cast method. These ZnO/PMMA nanocomposite films were then irradiated by swift heavy ion irradiation (Ni⁸⁺ ion beam, 100 MeV) at a fluence of 1×10¹¹ ions/cm². The nanocomposite films were then characterized by XRD, UV-vis absorption spectroscopy and photoluminescence spectroscopy. As revealed from the absorption spectra, absorption edge is not changed by the irradiation but the optical absorption is increased. Enhanced green luminescence at about 527 nm and a less intense blue emission peak around 460 nm were observed after irradiation with respect to the pristine ZnO/PMMA nanocomposite film.     

The effect of phonon anisotropic scattering on the thermal conductivity of silicon thin films at 300K and 400K

Previous studies have shown that anisotropy in phonon transport exist because of the difference in phonon dispersion relation due to different lattice directions, as observed by a difference in in-plane and cross-plane thermal conductivities. Our current work intends to study the effect of anisotropy scattering on silicon thermal conductivity at 300 K and 400 K. We adopt the Henyey and Greenstein probability density function in our phonon Monte Carlo simulation to investigate the effect of highly forward and backward scattering events. The impact of applying the anisotropy scattering using this approach is discussed in detail. While the forward and backward scattering will increase and decrease thermal conductivity respectively, the extent of the effect is non-linear such that forward scattering has a more obvious effect on thermal conductivity than backward scattering.