荧蒽／硬脂酸混合LB膜的时间分辨荧光研究

荧光法比吸光度法灵敏，更适用于超薄膜系如ＬＢ膜的表征。拉制了荧蒽和苯并［ｂ］荧蒽镶嵌在硬脂酸基质中的ＬＢ膜，探讨了它们的稳态和时间分辨荧光性质。实验表明，两种分子以单体形式存在于ＬＢ膜中。     

激光诱导时间分辨固体表面荧光光谱系统

采用斜射式激发样品光路结构,设计了应用于测试时间分辨固体表面荧光光谱系统。利用该系统研究了氧化锌薄膜在355 nm激光脉冲激发下的时间分辨固体表面荧光光谱。结果表明,该系统能够实现测量时间分辨固体表面荧光光谱,并由此测量了样品的固体表面荧光寿命。该系统结构简单可靠,灵敏度高,响应速度快。     

激光诱导时间分辨固体表面荧光光谱系统

采用斜射式激发样品光路结构,设计了应用于测试时间分辨固体表面荧光光谱系统。利用该系统研究了氧化锌薄膜在355 nm激光脉冲激发下的时间分辨固体表面荧光光谱。结果表明,该系统能够实现测量时间分辨固体表面荧光光谱,并由此测量了样品的固体表面荧光寿命。该系统结构简单可靠,灵敏度高,响应速度快。     

原油样品激光诱导荧光的时间分辨光谱特性研究

为探索激光诱导时间分辨荧光光谱技术应用于海洋悬浮溢油原位探测的可行性,对来自胜利油田六个不同井区不同密度的原油样品的时间分辨荧光光谱进行了探测分析。结果发现,各原油样品荧光发射的持续时间基本相同,从ICCD中数字延时发生器(DDG)的输入延时52 ns开始,到输入延时82 ns左右结束,各原油样品的荧光峰强度随时间变化曲线的半高宽约10 ns;不同原油样品的最强荧光峰位及其衰减寿命不尽相同,并且与样品密度有一定相关性,密度相近的原油具有相近的最强荧光峰位和相似的荧光寿命。对比六种原油样品的时间分辨荧光光谱发现,在荧光增强时,原油荧光光谱峰位不变,当荧光从最大强度开始衰减时,六种原油样品的荧光光谱峰位均出现了不同程度(17~30 nm)的红移现象,这一定程度上反映出原油中各荧光组分的荧光衰减速率存在差异,或者存在荧光组分之间的能量传递。所观测到的原油密度相关的时间分辨光谱信息和荧光峰红移现象可望成为水下悬浮溢油识别的有效特征之一。     

HpD肿瘤定位组份的时间分辨荧光光谱研究

采用微微秒激光作激发源的时间相关单光子计数系统测量了血卟啉衍生物的肿瘤定位组分(TLF)在缓冲液中不同阳离子表面活性剂浓度下的荧光衰减波形I(t)和时间分辨光谱I(λ,t).     

钐的时间分辨激光荧光光谱分析方法研究

本文利用Ｓｍ－ＴＴＡ－ＥｔＯＨ液体荧光体系，采用时间分辨激光荧光检测手段，建立了散的时间分辨光荧光分析法，该法的线性范围为０．０１～１０μｇ／ｍｌ，检出限为３．３ｎｇ／ｍｌ，０．５μｇ／ｍｌ钐标样测定的相对标准差为３．７％（ｎ＝１２），结合混合稀土中多种元素共存的特点，实验确定了装置的有关参数，用标准加入方法对实际样品进行了测定，并与其他方法测定结果进行了比较，结果满意，本法测定实际样品中钐的相对     

镝的时间分辨激光荧光光谱分析方法研究

围绕ＩＣＲＰ第６５号出版物的新建议，简述关于住宅和工作场所氡的防护问题，并回顾了氡研究热的历史、形成和发展，以及有关热点问题。     

激光诱导纳秒时间分辨荧光猝灭法原位研究菲及烷基菲与腐植酸相互作用

利用激光诱导纳秒时间分辨荧光(laser-induced nanosecond time-resolved fluorescence,LITRF)猝灭法原位研究腐植酸(humic acid,HA)分别与母环多环芳烃(polycyclic aromatic hydrocarbons,PAHs)菲(phenanthrene,Phe)及烷基PAHs 9-乙基菲(9-Ethylphenanthrene,9-EP)和惹稀(retene,Ret)相互作用,考察HA对母环及烷基PAHs结合特性差异与机制,对了解PAHs环境行为及生物有效性有重要意义。结果表明,通过改变延迟时间(50ns)可有效消除HA荧光干扰,实现游离Phe,9-EP及Ret浓度直接测定。利用Freundlich非线性等温吸附模型描述Phe,9-EP和Ret与HA结合特性,LITRF猝灭法与传统荧光法获得的模型拟合参数及单点结合系数结果一致。其中,参数n小于1,表明Phe,9-EP及Ret与HA均以非线性形式结合,且9-EP和Ret非线性程度高于Phe;相同给定平衡浓度下,HA与9-EP和Ret单点结合系数KOC大于Phe,而9-EP和Ret结合能力相近,且PAHs与HA结合系数均随给定浓度增加而降低。疏水性、取代基及与HA疏水空腔适应能力决定特定PAHs与HA结合特性。通过荧光寿命分析,HA存在下Phe,9-EP和Ret寿命分别为36.90,35.34和35.13ns,与未加入HA时的36.36,35.34和35.84ns无明显差异,表明Phe,9-EP和Ret与HA间的荧光猝灭以静态过程为主。LITRF猝灭法可快速有效原位研究PAHs与HA相互作用,有助于实现PAHs生态风险原位评估。     

联用多种荧光光谱研究高铁酸钾对荧蒽的降解

应用多种荧光光谱追踪了高铁酸钾对荧蒽的降解过程, 包括发射, 同步, 三维(EEM), 时间扫描及光度定量所提供丰富的关于整个降解反应的信息, 探讨了高铁酸钾对荧蒽分子的降解特性及其随时间变化规律; 分别对该降解过程中的不同时段(20, 40, 70 s)的时间扫描荧光曲线进行拟合,并由此推测了高铁酸钾降解荧蒽的动力学特征。结果显示, 相同的反应时段, 各荧光光谱反映的高铁酸钾对荧蒽分子的降解率非常接近: t=10 s约55%; t=25 s约81%; t=40 s约91%。各时段的降解过程中均未出现新的荧光特性; t≤20 s, 为该降解反应的决定性阶段, 此阶段的降解过程最为接近线性关系; t>20 s, 降解过程偏离线性关系越来越远。整个降解过程可以近似地用一级反应动力学规律描述。     

多环芳烃时间分辨荧光光谱特性研究

利用时间分辨荧光光谱技术,研究了菲、荧蒽、芴、蒽、芘等五种多环芳烃的荧光时间分辨发射光谱特性。以289 nm受激拉曼光作为激发光源,研究了289 nm激发光作用下五种多环芳烃的延时特性和门宽特性。并以多环芳烃随延时时间的荧光峰强度衰减关系曲线,得到菲、荧蒽、芴、芘的荧光寿命分别为37.0, 32.7, 10.9, 147.0 ns。不同荧光物质具有特定的荧光光谱特性,多环芳烃时间分辨荧光光谱特性的研究可以为复杂水体中不同种类多环芳烃的诊断提供依据。     

基于谷胱甘肽配体的ZnSe量子点对pH响应的时间分辨荧光光谱特性

当前,有关量子点pH响应方面的研究主要集中在含Cd(镉)类量子点,且都是研究其稳态荧光光谱对p H值的响应.然而,C d类量子点对生物体系具有一定的毒性,且稳态荧光光谱法由于受浓度等因素的影响具有一定的不稳定性,因此应用于生物体系中作为pH探针具有明显的缺点.基于以上分析,通过水相合成法,我们制备出了基于谷胱甘肽配体的...     

荧光光谱及其成像技术在光活检中的应用

分析了人体组织自体荧光的主要物质来源和荧光特性,同时总结了国内外常见的第二代新型光敏剂及其临床应用情况。在此基础上,全面比较了各种应用于早期肿瘤光活检的荧光光谱及其成像技术,并重点讨论了这些技术的基本原理和临床应用现状,以及它们今后的发展方向。     

葡萄球菌核酸酶蛋白的时间分辨荧光与热力学特性

葡萄球菌核酸酶(SNase)是一种小型球状蛋白,其变体常用来研究蛋白质的折叠过程。不同于之前报道的研究方法和技术手段,采用时间相关单光子计数(TCSPC)及飞秒荧光上转换技术,结合紫外吸收谱和稳态荧光光谱,研究了SNase蛋白变体Δ+PHS和Δ+PHS+I92A的荧光动力学,以及不同温度下蛋白结构与热稳定性的关系,证明蛋白质内色氨酸残基可作为一种内源性探针对蛋白变体的结构折叠和热稳定性进行印证和研究。衰减相关光谱(DAS)表明了两种变体随温度变化的不同趋势,在此基础上进一步分析了这两种变体的结构折叠及热稳定性的差异。皮秒时间分辨发射光谱(TRES)显示色氨酸残基存在0.5 ns的连续光谱弛豫过程,而光谱移动量可作为SNase变体蛋白结构紧密程度的判断依据。飞秒上转换数据分析结果中,0.5 ps的DAS在光谱蓝端为正、红端为负,表明了色氨酸残基受到弛豫效应的影响。200 ps的寿命则说明色氨酸残基与周围猝灭基团之间存在电子转移过程。时间分辨荧光各向异性(anisotropy)的分析结果则说明了色氨酸残基在蛋白质体系内具有独立的局部运动,且其强弱与变体的热稳定性和热运动的整体效果有关。测量和分析色氨酸残基的时间分辨荧光性质为深入研究SNase蛋白的结构和功能提供了新的思路。     

基于激光诱导时间分辨荧光的原油识别方法研究

在柴油、汽油、重质燃料油等成品油和原油等溢油油源的区分方面,荧光光谱结合模式识别手段得到了广泛的应用。传统的三维荧光光谱分析方法虽然能够获得溢油样品丰富的成分信息,但难以适应现场应用的要求,目前还停留在实验室检测的阶段。发展适用于现场应用的原油识别方法,对于海洋溢油污染的快速响应与处理意义重大。面向激光雷达的需要,发展了一种基于激光诱导时间分辨荧光手段、结合支持向量机（SVM）模型的原油识别方法,从时间和波长两个不同维度出发,通过对时间窗口和波长范围的选取进行优化,获得了理想的油种识别准确率。实验结果表明通过选取ICCD探测延时为54～74 ns可以将分类正确率从全谱线数据的83.3%提高到88.1%。通过选取波长范围为387.00～608.87 nm的谱线数据,可将疑似油种的分类正确率从全谱线数据的84%提高到100%。激光荧光雷达在实际工作中,受波浪、运载平台晃动等因素的影响,探测延时会出现一定的波动。本文介绍的分类识别方法通过时间和波长两个维度的筛选,更加适用于现场探测数据的识别,并进一步凸显了原油时间分辨荧光光谱特征,为疑似油种分类识别过程中数据量的压缩提供了重要依据。     

Time-Resolved Fluorescence Spectroscopy Study on the Photophysical Behavior of Quantum Dots

Room-temperature time-resolved luminescence measurements on single CdSe/ZnS quantum dots (QDs) are presented. Fluorescence emission spectra were recorded over periods of up to 30 minutes with a time resolution as small as 6 ms. For QDs in ambient air, a clear 30–40 nm blue shift in the emission wavelength is observed, before the luminescence stops after about 2–3 minutes because of photobleaching. In a nitrogen atmosphere, the blue shift is absent while photobleaching occurs after much longer times (i.e., 10–15 minutes). These observations are explained by photoinduced oxidation. The CdSe surface is oxidized during illumination in the presence of oxygen. This effectively results in shrinkage of the CdSe core diameter by almost 1 nm and consequently in a blue shift. The faster fading of the luminescence in air suggests that photoinduced oxidation results in the formation of non-radiative recombination centers at the CdSe/CdSeO_x interface. In a nitrogen atmosphere, photoinduced oxidation is prevented by the absence of oxygen. Additionally, a higher initial light output for CdSe/ZnS QDs in air is observed. This can be explained by a fast reduction of the lifetime of the long-lived defect states of CdSe QDs by oxygen.     

Quantitative Time-Resolved Fluorescence Spectrum of the Cortical Sarcoma and the Adjacent Normal Tissue

The difference in time-resolved fluorescence spectrum between the cortical sarcoma and the adjacent normal tissue was studied in both experimental and theoretical ways. The Clinical data were obtained in vivo using a time-resolved fluorescence spectrometer employing a single fiber-optic probe for excitation and detection. Tissue was modeled as s-180 sarcoma tumor surrounded with normal muscle and was mediated by the Palladium-porphyrin photosensitizer (Pd-TCPP). The emitted fluorescence was considered as arising from the tumor tissue or the normal muscle, due to the presence of the photosensitizer. A computational code which could simulating time-resolved fluorescence emission was presented and applied to comparing fluorescence decay of photosensitizer in different stages of tumor growth. In this code the different stages of the tumor was modeled through changing the time τ, the delay of the fluorescence photon emission and z _max, the thickness of the tumor. It was found in the in vivo experiment that the fluorescence from tumor tissue decayed more quickly than from the adjacent normal muscle. For the ten rats in the first experiment day, the mean decay constant of tumor T _s and normal tissue T _n were 554 and 526 μs, respectively. And T _s increased with the tumor growth, from 554 μs in the first day to 634 μs in the eighth day while T _s kept steady. It was believed that the more adequate oxygen supplied by the normal tissue can more effectively quench the fluorescence and in the normal tissue the photosensitizer lifetime is smaller. As a result the simulated time-resolved fluorescence spectrum of normal tissue showed more quickly decay. And the thickness of the tumor can also delay the fluorescence decay. Both the experimental and simulated results indicated that the germination of the tumor would increase the decay constant of the time-resolved fluorescence spectrum. So decay constant of the tumor tissue spectrum should be larger than that of adjacent normal tissue for the reason of hypoxia and overgrouth. This fact could be of use in the tumor diagnoses.     

Steady-State and Time-Resolved Fluorescence Polarization Behavior of Acenaphthene

Steady-state and time-resolved fluorescence polarization studies have been carried out on acenaphthene (ACE) in low-temperature glass solutions and at room temperature. In the low-temperature glass the fluorescence polarization values vary considerably with both emission and excitation wavelength. There is a time dependence (on the nanosecond time scale) of the fluorescence anisotropy, r(t), at 77 K, which has a strong dependence upon the excitation and emission wavelengths. Under these conditions, the time-dependent decay of the anisotropy is not attributable to chromophoric motion. The observations are consistent with emission from two closely lying and interconverting excited states. Rate constants for the photophysical processes involved have been determined by fitting the data using a model proposed by Fleming et. al. The results are discussed with particular reference to the care required in using dynamic fluorescence polarization measurements to determine energy transfer rates in systems containing this chromophore.     

激光诱导的钛酸钡等离子体的时间分辨光谱

利用光学多通道分析仪（ＯＭＡⅢ）研究脉冲激光沉积钛酸钡薄膜过程中的激光诱导等离子体的时间分辨发射光谱，利用各种粒子不同时刻发射的谱线强度描绘成该粒子的飞行时间谱，表征了等离子体中该粒子的空间浓度分布，根据飞行时间谱的特征，推算了粒子束脉冲（等离子体）的空间宽度及其与缓冲气体压力的关系，提出了在激光沉积多元氧化物薄膜过程中的合适的缓冲气体压力范围，解释了激光原位沉积高温超导薄膜中所需氧气分压达３０Ｐ