曙红B荧光猝灭法测定司帕沙星

基于司帕沙星对曙红 B的荧光具有猝灭特性 ,建立一种测定微量司帕沙星的方法。在 p H=3.5的Clark- Lubs缓冲溶液中 ,曙红 B激发波长 λex=30 8nm、发射波长 λem=5 40 nm,司帕沙星的浓度在 0 .2—4 mg· L-1范围内符合比耳定律 ,相关系数为 0 .997,检出限为 0 .0 5 4mg· L-1。该方法对胶囊中的司帕沙星进行回收 ,回收率为 90 %— 10 9% ,相对标准偏差为 1.2 %— 2 .8%。猝灭机理的初步研究 ,认为主要是静态猝灭 ,求得司帕沙星与曙红 B的结合常数为 7.94× 10 4,结合比为 1.0 2。     

光谱学 其他

O657.39 2006031939流动注射化学发光法测定司帕沙星的研究=Chemilumi-nescence determination of Sparfloxacin by flowinjection a-nalysis[刊,中]/石杰(郑州大学化学系.河南,郑州(450052)) ,曹丰璞…∥分析试验室.—2006 ,25(3) .—89-91采用流动注射技术,建立了一种简单、快速测定司帕沙星的方法。线性范围为1 .0×10-7~8 .5×10-4mol/L,检出限为6 .5×10-8mol/L。利用该法测定了司帕沙星片剂中的司帕沙星,回收率在98 .8 %~104 .4 %之间。图1表2参12(严寒)O657.39 2006031940流动注射化学发光法测定褪黑素=Determination of me-laton…     

荧光法研究司帕沙星与白蛋白的作用

本文用荧光光谱法、分光光度法研究了水溶液中喹诺酮类药物司帕沙星与牛血清白蛋白 (BSA)、鸡蛋白 (CEA)的相互作用 ,求得它们间的结合常数为K鸡 =8 2 9× 10 6,K牛 =4 41× 10 7;结合位点数分别为n鸡=0 5 88,n牛 =0 793,并根据F rster非辐射能量转移机制 ,测定了司帕沙星与两种血清白蛋白相互结合时其给体 受体间距离 (R鸡 =1 99nm ,R牛 =2 0 9nm)和能量转移效率 (E鸡 =0 76 6 ,E牛 =0 714)。实验表明 ,随着温度升高 ,BSA及CEA的猝灭曲线斜率降低 ,证实了司帕沙星与BSA和CEA的相互结合作用为单一的静态猝灭过程 ,其作用机制属能量转移机制。通过两种血清白蛋白与抗菌药物司帕沙星结合反应 ,探讨了药物司帕沙星在生物体内与蛋白质的相互作用的生物学效应及其作用机理。     

司帕沙星氯代物的制备及荧光性质研究

司帕沙星在酸性介质中与亚硝酸反应 ,其重氮盐在氯化亚铜存在下 ,继而与氢氯酸反应生成一种较司帕沙星荧光响应值高 1 1 0倍的强荧光物质 ,采用元素分析、红外光谱和质谱对其衍生物的结构进行了表征。结果表明 ,司帕沙星的荧光强度与其喹啉环 5 位上的氨基密切相关 ,本文还对司帕沙星的荧光自猝灭及氯代荧光增敏机理进行了探讨。     

对硝基酚分光光度法测定氯氮卓的含量

本文主要研究在硼砂水溶液中 ,氯氮卓与对硝基酚发生荷移反应 ,生成稳定的 1∶ 1络合物。络合物的最大吸收波长为 4 35 nm,表观摩尔吸光系数 ε=3.83× 10 3L·mol-1·cm-1。基于以上反应 ,本方法测定氯氮卓药物制剂含量与文献值基本一致 ,回收率为 99.61%— 10 0 .10 % ,相对标准偏差为 0 .64%     

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％.     

亚叶酸钙与对硝基酚荷移反应的研究

本文主要研究了在水溶液中亚叶酸钙与对硝基酚发生荷移反应生成稳定的 1∶ 1络合物 ,络合物的最大吸收波长为 4 0 2 .2 nm,表观摩尔吸光系数为 ε=5 .2 5 5× 10 2 L· mol-1· cm-1,线性范围为 5 0—12 0 0 μg/ m L。回收率为 99.5 8%— 10 2 .6 0 % ,相对标准偏差为 1.4 3%。方法简单、快速、准确度高 ,可用于亚叶酸钙制剂含量的测定。     

碘蓝分光光度法测定微量铬（Ⅳ）

基于在酸性介质中 ,重铬酸钾与碘化钾、淀粉的显色反应 ,建立了碘蓝分光光度法测定微量铬 ( )的方法。铬 ( )浓度在 0— 0 .6μg/ m L范围内有良好的线性关系 ,方法的相对标准偏差为 1.3% ,表观摩尔吸光系数为 5 .6 3× 10 4 L· mol- 1 · cm- 1 ,检出限为 2 .0× 10 - 3μg/ m L     

对硝基酚荷移分光光度法测定甲氧苄啶的含量

在水溶液中甲氧苄啶与对硝基酚发生反应生成 1∶ 1的荷移络合物。络合物最大吸收波长 4 0 2 .4 nm,线性范围 2— 2 5 μg/ m L,表观摩尔吸光系数为 ε=8.4 6 8× 10 3 L· mol-1· cm-1,回收率为99.6 7%— 10 0 .4 % ,相对标准偏差为 1.3% (n=5 )。本法测定甲氧苄啶药物制剂含量 ,结果令人满意。     

紫外分光光度法测定司帕沙星注射液主含量

紫外分光光度法测定乳酸司帕沙星葡萄糖注射液的含量。司帕沙星浓度在2—12μg／mL范围内与吸光度呈良好的线性关系。回收率为99．8％-100．1％，RSD为0．1％。该法简便、快速，重复性好，结果准确可靠。     

Guided-Wave Two-Dimensional Acousto-Optic Scanner Using Proton-Exchanged Lithium Niobate Waveguide

Two-dimensional scanning of a 0.6328 mum guided-light beam has been realized using noncolinear acousto-optic (AO) coplanar Bragg diffraction together with colinear AO guided-mode to substrate radiation-mode conversion in a Z-cut Xpropagation LiNbO3 proton-exchanged (PE) waveguide. The two surface acoustic (SAW) waves utilized are at the center frequencies of 500 and 200 MHz, propagating in the Y and X axes, respectively. Two-dimensional scanning of approximately 720 resolvable light beam spots, namely, 18 40 (horizontal vertical) scanning, has been demonstrated using a light beam of 1.0 mm aperture. The total number of resolvable beam spots can be greatly increased from 720 by simply utilizing SAW transducers of larger bandwidth and a light beam of greater aperture. It should also be possible to significantly increase the diffraction efficiency from 3 % by optimizing the parameters of the PE waveguide and the SAWs.     

Effect ofγ-radiation on the spectral luminescence characteristics of impure cadmium tungstate crystals

Results of a study of the effect of γ-radiation on the spectral luminescence properties of cadmium tungstate crystals doped with silver, bismuth, and molybdenum cations are presented. Spectral characteristics of the nondnnnoped crystals are briefly described. Absorption and photo and X-ray luminescence spectra of the crystals taken before and after exposure to γ-radiation (5.5·10⁴ Gy) are compared. It is found that the spectral characteristics of the crystals doped with silver, bismuth, and molybdenum cations do not change markedly after the exposure. The relation between the type of impurity-induced defects, individual characteristics of the impurity cations, and the character of the effect of γ-radiation on the spectral luminescence properties of impure crystals is analyzed (preliminarily). Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 64, No. 1, pp. 55–60, January–February, 1997.     

Measurement of nonlinear coefficient of optical fiber based on small chirped soliton transmission

We measure the waveform and phase curves of short optical pulses before and after transmission over different lengths of fibers by use of the pulse analyzer with the frequency-resolved optical gating (FROG),and numerically simulate pulse evolution under the experimental conditions.The nonlinear coefficient of the fiber is given by comparing the experimental results with the numerical ones.Difference between the experiment and numerical simulation is analyzed.     

Resonance scattering of canonical elastic shells in absorbing fluid medium

Resonance scattering of elastic spherical shell and cylindrical shell while the surrounding fluid medium has absorption is studied. The normal mode solution derived using exact elastic theory and the separation of variables is still applicable. However, the scattering form function has to be modified for the absorbing medium, otherwise the unreasonable result would be obtained. The backscattering form function in the absorbing medium is redefined, and the form function of elastic spherical and cylindrical shell with vacuum or solid matter filled is calculated in various absorption conditions. The results show that the absorption of surrounding fluid leads to notable attenuation of the coincidence resonances in the mid-frequency, but it has a little influence on the low-frequency resonance scattering induced by the filler inside the shell.     

Single-beam self-referenced phase-sensitive surface plasmon resonance sensor with high detection resolution

A versatile and low-cost single-beam self-referenced phase-sensitive surface plasmon resonance(SPR)sensing system with ultra-high resolution performance is presented.The system exhibits a root-mean-square phase fluctuation of ±0.0028.over a period of 45 min.i.e.a resolution of±5.2×10-9 refractive index units.The enhanced performance has been achieved through the incorporation of three design elements:a true single-beam configuration enabling complete self-referencing so that only the phase change associated with SPR gets detected,a differential measurement scheme to eliminate spurious signals not related to the sensor response,and the elimination of retardation drifts by incorporating temperature stabilization in the liquid crystal phase modulato .Our design should bring the detection sensitivity of non-labeling SPR biosensing closer to that achievable by conventional fluorescence-based techniques.     

Influences of SiO2 protective layers and annealing on the laser-induced damage threshold of Ta2O5 films

Ta2O5 films are prepared on BK7 substrates with conventional electron beam evaporation deposition.The effects of SiO2 protective layers and annealing on the laser-induced damage threshold (LIDT) of the films are investigated.The results show that SiO2 protective layers exert little influence on the electric field intensity(EFI)distribution,microstructure and microdefect density but increase the absorption slightly.Annealing iS effective on decreasing the microdefect density and the absorption of the films.Both SiO2 protective layers and annealing are beneficial to the damage resistance of the films and the latter is more effective to improve the LIDT.Moreover,the maximal LIDT of Ta2O5 films is achieved by the combination of SiO2 protective layers and annealing.     

A stereo matching algorithm using multi-peak candidate matches and geometric constraints

Gray cross correlation matching technique is adopted to extract candidate matches with gray cross correla- tion coefficients less than some certain range of maximal correlation coefficient called multi-peak candidate matches. Multi-peak candidates are extracted corresponding to three closest feature points at first. The corresponding multi-peak candidate matches are used to construct the model polygon. Correspondence is determined based on the local geometric relations between the three feature points and the multi-peak candidates. The disparity test and the global consistency checkout are applied to eliminate the remaining ambiguous matches that are not removed by the local geometric relational test. Experimental results show that the proposed algorithm is feasible and accurate.     

Fiber Modal Index Measurements Based on Fiber Gratings

A novel method based on fiber gratings for measuring the effective indices of fiber modes is proposed. The effective index difference between the core mode and a cladding mode was obtained by analyzing the interference fringe of a pair of cascaded long-period fiber gratings. In order to extract the core mode index from the measured index difference, an index matching oil immersion method is proposed. By analyzing the interaction between the cladding mode and the oil applied on the cladding surface, the mode order and the effective index of the involved cladding mode might be calculated. Experimental results about the interference fringe shifts induced by the oil index and the oil-applied length are also presented.     

Optical Pulse Compression Schemes That Use Nonlinear Bragg Gratings

Nonlinear optical pulse compression of picosecond pulses typically requires long lengths of optical fiber and multiple components. Periodic structures, such as fiber Bragg gratings, are highly dispersive at wavelengths outside of the photonic bandgap. This implies that such gratings can be used as very short all-fiber compressors. In this paper a number of such compression schemes are reviewed involving uniform and nonuniform fiber Bragg gratings, relying on both soliton and nonsoliton compression principles. Experimental results supporting the corresponding underlying theory are also presented. Finally, an extension of one of the compression schemes is shown, which allows the generation of adjustable high-repetition rate soliton trains.