基于荧光强度快速判断蛋白可溶性方法的建立

目的:建立一种通过观察荧光强度,快速、直观地判断蛋白可溶性的方法。方法:选择抗辐射蛋白CBL502-AA及其突变体CBL502-ΔAA′作为目的蛋白,增强型绿色荧光蛋白作为报告分子,分别构建融合蛋白表达载体;通过SDS-PAGE和荧光观察两种手段检测和比较融合蛋白的可溶性。结果:荧光观察融合蛋白的可溶性与SDS-PAGE检测结果一致。结论:建立了一种基于荧光强度,快速、简单、直观的比较蛋白可溶性的方法。     

毫微秒荧光谱仪的自动数据处理系统

本文描述了时间相关单光子毫微秒荧光谱仪的自动数据处理系统,介绍了它的工作原理、设计特点及其应用。     

抗砷细胞荧光染色后的激光共聚焦显微镜检测

目的:应用激光共聚焦显微镜检测活细胞内荧光物质含量.方法:传代培养长期低剂量砷诱导的抗砷细胞,用荧光染料Rhodamine-123对细胞染色30min,实验组与维拉帕米(Verapamil)共同孵育,对照组为单加Rhodamine-123的抗砷细胞.应用激光共聚焦显微镜采集Rhodamine-123的荧光图像动态序列,并且记录不同时间段的细胞内荧光强度.结果:实验组细胞染色12h,24h,36h,48h,60h后,荧光强度依次为(51.567±0.7572)、(46.533±0.7095)、(39.557±0.601)、(38.6±0.6245)和(38.505±0.718),明显高于同时间段对照组的荧光强度,差异均有显著性(P＜0.01).结论:应用激光共聚焦显微成像技术能进行活细胞水平荧光物质实时定量检测.     

基于荧光方法的大肠杆菌单管定量检测技术研究

通过研究培养温度、培养基pH值对大肠杆菌生长和培养液荧光强度的影响,确定44℃,培养液pH值7.0～7.5为大肠杆菌MUG酶荧光检测的最佳条件。通过研究培养时间和接种菌浓度与培养液荧光强度的关系,建立起基于荧光方法检测大肠杆菌的单管定量检测技术。通过与平板菌落计数法和最大可能数法比较发现单管定量检测法的相对标准偏差小于这两种常用的方法,而且更为快速、经济,适合用于大肠杆菌的定量检测。     

一种提高质粒DNA凝胶电泳检测灵敏度的方法

比较了凝胶电泳示检测质粒ＤＮＡ时不同激发波长对ＤＮＡ－ＥＢ荧光强度的影响,发现短波长激发光可增加ＤＮＡ的探测灵敏度。采用２６０ｎｍ作为激光光时可探测到少至０．７ｎｇ的线性ＤＮＡ。且在很广的ＤＮＡ的质量范围内,ＤＮＡ－ＥＢ荧光强度 与ＤＮＡ量或正比。以此改进方法检测电离辐射诱导的ＤＮＡ单、双链断裂岢得到与其它研究结果相一致的Ｇ（ＳＳＢ）和Ｇ（ＤＳＢ）值。     

超短脉冲技术测量癌细胞荧光光谱与荧光寿命

研究用于癌症诊断与治疗的光敏剂血卟啉（hematoporphyrin derivative,HPD）的超快光动力学过程,采用超短脉冲激光光谱技术和皮秒时间相关单光子计数系统,测量经血卟啉培养的活体癌细胞与正常细胞的荧光光谱、荧光寿命特性及荧光峰值强度随时间变化曲线,并测量单一细胞内部不同位置的荧光寿命特性,观测到：癌细胞样品在645 nm处具有特有的光谱谱峰;癌细胞样品荧光寿命的快成分约150 ps慢成分约1200 ps,而正常细胞样品快成分约300 ps慢成分约2500 ps;癌细胞样品的荧光峰值强度经12小时衰减约10%,而正常细胞样品衰减约55%;在细胞内部荧光寿命300 ps的快成分十分显著,且中心部位血卟啉浓度最高.癌细胞与正常细胞的荧光光谱、荧光寿命特性及荧光峰值强度随时间变化曲线相差十分明显,反映了癌细胞与正常细胞对血卟啉亲和特性有显著的差异,测量结果确认了荧光光谱技术诊断与治疗癌症的可行性,并对发展超短脉冲激光光谱技术早期诊断与治疗癌症具有重要的指导意义和临床应用价值.     

非水介质中辣根过氧化物酶（HRP）荧光活性测定法

建立了一种分析ＨＲＰ催化活力的新方法。该方法基于单体（底物）、聚合物（产物）的荧光发射光谱不重叠,使用荧光光谱仪,通过测量底物荧光淬灭来检测ＨＲＰ在非水介质中（二氧六环－水、乙醇－水、丙酮－水体系）催化酚类、芳香胺类物质聚合的活力。此方法迅速、简便,结果是定量并可重复的,并能定量地计算底物转化率。     

用于浮游植物探测的三维激光诱导荧光光谱系统

本文介绍一个针对浮游植物现场探测的三维激光诱导荧光（3D-LIF）光谱系统。该系统以波长可调谐激光器为光源,使用光栅光谱仪进行光谱分光,输出光谱范围380 nm ～800 nm,并选用32通道光电倍增管模组作为光电探测器。光栅光谱仪和光电倍增管模组之间的耦合选用芯径0．2 mm 的光纤束,对应光谱分辨率约为3 nm,以此采集接收的31通道发射荧光光谱,其光谱范围为410 nm ～710 nm,光谱带宽约10 nm。光电转换电路的模拟带宽约为20 MHz,数据采集频率50 MHz,分辨率14 bit。基于研发的光谱系统,采用光学参量放大器（OPO）以获得405 nm ～615 nm 可调谐激发光源,在实验室对三十余种中国海常见的浮游植物的3D-LIF 光谱进行了测量。测量结果证实了系统的稳定性和用于藻种分类和识别研究的有效性。系统中的激光器和望远镜可灵活更换,接收的光谱范围和光谱分辨率等参数可便利调节,因此,该系统可望发展成为用于现场探测的3D-LIF 光谱系统。     

草鱼出血病病毒多肽的荧光染色

将草鱼出血病病毒（ＧｒａｓｓＣａｒｐＨｅｍｏｒｒｈａｇｅＶｉｒｕｓ,ＧＣＨＶ）置于还原性的溶液中,然后加入等体积的ＮａＨＣＯ３配制的异硫氰酸荧光索溶液进行多肽的标记,再经ＳＤＳ－ＰＡＧＥ分析,在紫外灯下即可检测到ＧＣＨＶ全部的１１个结构多肽的荧光带。该方法最小检测量为５００ｎｇ,由该方法回收的多肽具有抗原活性,可作为抗原进行免疫学实验。     

定量荧光原位杂交测定端粒长度

目的:应用定量荧光原位杂交(Q-FISH)方法测定端粒长度。方法:选取4种端粒长度均一的标准细胞株采用Q-FISH的方法做出荧光亮度与端粒长度的标准曲线,从而得出实验细胞株的端粒长度,与DNA印迹法测定末端限制性片段(TRF)长度进行二者之间的相关性分析。结果:检测荧光强度的最佳线性曝光时间为400ms,相对于DNA印迹法,定量荧光原位杂交(Q-FISH)法所需标本量少,实验周期短,端粒长度结果与Southern杂交法具有很好的相关性。结论:采用定量荧光原位杂交方法测端粒长度具有重复性好、精确可靠的特点,适用于对珍贵标本的端粒改变进行分析。     

Measuring Spray Droplet Size from Agricultural Nozzles Using Laser Diffraction

When making an application of any crop protection material such as an herbicide or pesticide, the applicator uses a variety of skills and information to make an application so that the material reaches the target site (i.e., plant). Information critical in this process is the droplet size that a particular spray nozzle, spray pressure, and spray solution combination generates, as droplet size greatly influences product efficacy and how the spray moves through the environment. Researchers and product manufacturers commonly use laser diffraction equipment to measure the spray droplet size in laboratory wind tunnels. The work presented here describes methods used in making spray droplet size measurements with laser diffraction equipment for both ground and aerial application scenarios that can be used to ensure inter- and intra-laboratory precision while minimizing sampling bias associated with laser diffraction systems. Maintaining critical measurement distances and concurrent airflow throughout the testing process is key to this precision. Real time data quality analysis is also critical to preventing excess variation in the data or extraneous inclusion of erroneous data. Some limitations of this method include atypical spray nozzles, spray solutions or application conditions that result in spray streams that do not fully atomize within the measurement distances discussed. Successful adaption of this method can provide a highly efficient method for evaluation of the performance of agrochemical spray application nozzles under a variety of operational settings. Also discussed are potential experimental design considerations that can be included to enhance functionality of the data collected.     

时间分辨荧光光谱测量结果的一种数据处理改进方法

在综合矩方法和拉普拉斯变换方法原理的基础上,本文报道一种时间相关单光子计数测出的荧光衰变动力学曲线的数据处理的改进方法.此方法使我们能在花费时间较少的条件下得出和用最小二乘法拟合相比拟的准确分析结果.这一方法的优点已被用于分析香豆素102+DCM和香豆素102+PBBO激光染料乙醇溶液的双指数荧光衰变过程的结果所证实,此外,本文也讨论了仪器时间漂移校正及拉普拉斯变换的数据截取问题.     

Laser spectroscopic assessment of induced hyperoxia--an animal experiment in lambs

The noninvasive determination of biochemical parameters has become an important aspect of intensive care medicine. The newly developed monitors for laser reflectometry provide the possibility of spectroscopic monitoring. The equipment consists of a near-infrared data collection unit and a personal computer. The four laser diodes emit light at wavelengths of 775, 805, 845 and 904 nm. By analyzing the changes in optical density during laser irradiation of biological tissue, information is obtained about the relative changes in the concentration of hemoglobin and the blood volume. In animal experiments with ten fetal lambs we evaluated the reliability of near infrared laser spectroscopy. Fetal hyperoxia was achieved by means of an extracorporeal circuit with interposition of a membrane oxygenator (0.8 m2, Scimed). During the induced hyperoxia the laser spectroscopic tracings showed a rise in the HbO2 signal with a synchronous decrease in the HbR signal. Additionally, the spectroscopic pattern showed a characteristic initial rise in the intracerebral blood volume, which stabilized after 4 minutes. We found a significant correlation between the intermittently measured PO2 values of the arterial blood samples and the laser spectroscopic HbO2 and HbR signals (r = 0.87, and r = -0.82, respectively; p less than 0.001). Furthermore, hyperoxia was indicated by the laser system with a short lag time. We conclude that laser spectroscopy is a reliable method with a high potential for clinical routine use in intensive care, as it provides noninvasive continuous information at comparatively low costs using portable monitors.     

Evaluation of confocal microscopy system performance

BACKGROUND: The confocal laser scanning microscope (CLSM) has been used by scientists to visualize three-dimensional (3D) biological samples. Although this system involves lasers, electronics, optics, and microscopes, there are few published tests that can be used to assess the performance of this equipment. Usually the CLSM is assessed by subjectively evaluating a biological/histological test slide for image quality. Although there is a use for the test slide, there are many other components in the CLSM that need to be assessed. It would be useful if tests existed that produced reference values for machine performance. The aim of this research was to develop quality assurance tests to ensure that the CLSM was stable while delivering reproducible intensity measurements with excellent image quality. METHODS: Our ultimate research objective was to quantify fluorescence using a CLSM. To achieve this goal, it is essential that the CLSM be stable while delivering known parameters of performance. Using Leica TCS-SP1 and TCS-4D systems, a number of tests have been devised to evaluate equipment performance. Tests measuring dichroic reflectivity, field illumination, lens performance, laser power output, spectral registration, axial resolution, laser stability, photomultiplier tube (PMT) reliability, and system noise were either incorporated from the literature or derived in our laboratory to measure performance. These tests are also applicable to other manufacturer's systems with minor modifications. RESULTS: A preliminary report from our laboratory has addressed a number of the QA issues necessary to achieve CLSM performance. This report extends our initial work on the evaluation of CLSM system performance. Tests that were described previously have been modified and new tests involved in laser stability and sensitivity are described. The QA tests on the CLSM measured laser power, PMT function, dichroic reflection, spectral registration, axial registration, system noise and sensitivity, lens performance, and laser stability. Laser power stability varied between 3% and 30% due to various factors, which may include incompatibility of the fiber-optic polarization with laser polarization, thermal instability of the acoustical optical transmission filter (AOTF), and laser noise. The sensitivity of the system was measured using a 10-microm Spherotech bead and the PMTs were assessed with the CV concept (image noise). The maximum sensitivity obtainable on our TCS-SP1 system measured on the 10-microm Spherotech beads was approximately 4% for 488 nm, 2.5% for 568 nm, 20% for 647 nm, and 19% for 365 nm laser light. The values serve as a comparison to test machine sensitivity from the same or different manufacturers. CONCLUSIONS: QA tests are described on the CLSM to assess performance and ensure that reproducing data are obtained. It is suggested strongly that these tests be used in place of a biological/histological sample to evaluate system performance. The tests are more specific and can recognize instrument functionality and problems better than a biological/histological sample. Utilization of this testing approach will eliminate the subjective assessment of the CLSM and may allow the data from different machines to be compared. These tests are essential if one is interested in making intensity measurements on experimental samples as well as obtaining the best signal detection and image resolution from a CLSM. Published 2001 Wiley-Liss, Inc.     

用光声技术测量生物组织粘弹特性的研究

报道了一种用光声技术测量生物组织粘弹特性的新方法,即用脉冲激光在生物组织中激发出光声信号（应力波）,从光声信号的振幅弛豫特性曲线中测量出应力波的弛豫时间,根据粘弹性理论,该弛豫时间就等于生物组织的粘弹比.用该方法测量Kelvin-Voigt模型的模拟生物组织的粘弹比,测量结果与用流变仪测量的结果完全一致,符合率达到97%.进而用光声方法测量出Maxwell模型的生物组织的粘弹比.理论分析与实验结果都表明：该方法只与被测物的声阻抗有关,而与它的状态无关,因此可用于任意状态的生物组织粘弹特性的测量.光声测量方法具有实时、快速、测量灵敏度高和重复性好的优点,因此在生物医学领域具有潜在的应用前景.     

Characterizing Far-infrared Laser Emissions and the Measurement of Their Frequencies

The generation and subsequent measurement of far-infrared radiation has found numerous applications in high-resolution spectroscopy, radio astronomy, and Terahertz imaging. For about 45 years, the generation of coherent, far-infrared radiation has been accomplished using the optically pumped molecular laser. Once far-infrared laser radiation is detected, the frequencies of these laser emissions are measured using a three-laser heterodyne technique. With this technique, the unknown frequency from the optically pumped molecular laser is mixed with the difference frequency between two stabilized, infrared reference frequencies. These reference frequencies are generated by independent carbon dioxide lasers, each stabilized using the fluorescence signal from an external, low pressure reference cell. The resulting beat between the known and unknown laser frequencies is monitored by a metal-insulator-metal point contact diode detector whose output is observed on a spectrum analyzer. The beat frequency between these laser emissions is subsequently measured and combined with the known reference frequencies to extrapolate the unknown far-infrared laser frequency. The resulting one-sigma fractional uncertainty for laser frequencies measured with this technique is ± 5 parts in 10⁷. Accurately determining the frequency of far-infrared laser emissions is critical as they are often used as a reference for other measurements, as in the high-resolution spectroscopic investigations of free radicals using laser magnetic resonance. As part of this investigation, difluoromethane, CH₂F₂, was used as the far-infrared laser medium. In all, eight far-infrared laser frequencies were measured for the first time with frequencies ranging from 0.359 to 1.273 THz. Three of these laser emissions were discovered during this investigation and are reported with their optimal operating pressure, polarization with respect to the CO₂ pump laser, and strength.     

Research on Laser Marking Speed Optimization by Using Genetic Algorithm

Laser Marking Machine is the most common coding equipment on product packaging lines. However, the speed of laser marking has become a bottleneck of production. In order to remove this bottleneck, a new method based on a genetic algorithm is designed. On the basis of this algorithm, a controller was designed and simulations and experiments were performed. The results show that using this algorithm could effectively improve laser marking efficiency by 25%.     

二氧化碳安乐死在实验动物中的应用与最新进展

本文概述了二氧化碳（CO2）安乐死法的作用机制、CO2使用浓度、应用范围和操作注意事项,并讨论了该方法的动物福利、设备改进等问题。     

激光针灸对穴位组织温度和血流灌注率的影响

本文在Pennes方程的基础上研究了激光针灸治疗对穴位组织的温度和血流灌注率的影响。结果显示,连续激光与脉冲激光针灸都能使穴位组织的温度和血流灌注率升高,随着激光的功率密度升高则穴位组织的温度和血流灌注率亦升高。通过这些研究为激光针灸的临床实际应用提供了理论基础。     

Analysis of the electron transfer from Pheo to QA in PS II membrane fragments from spinach by time resolved 325 nm absorption changes in the picosecond domain

Absorption changes at 325 nm (delta A325) induced by 15 ps laser flashes (lambda = 650 nm) in PS II membrane fragments were measured with picosecond time-resolution. In samples with the reaction centers (RCs) kept in the open state (P I QA) the signals are characterized by a very fast rise (not resolvable by our equipment) followed by only small changes within our time window of 1.6 ns. In the closed state (PI QA-) of the reaction center the signal decays with an average half-life time of about 250 ps. It is shown that under our excitation conditions (E = 2 x 10(14) photons/cm2 per pulse) subtraction of the absorption changes in closed RCs (delta A closed 325) from those in open RCs (delta A open 325) leads to a difference signal which is dominated by the reduction kinetics of QA. From the rise kinetics of this signal and by comparison with data in the literature it is inferred that QA becomes reduced by direct electron transfer from Pheo- with a time constant of about 350 +/- 100 ps.