贵金属纳米结构为敏感层的锥形光纤探针及其SERS活性

表面等离激元纳米结构与便携式光纤拉曼系统相结合,在液体样品和生物活体组织的快速、实时监测上有较好的应用前景。其核心技术是将具有表面增强拉曼散射(SERS)活性的贵金属纳米结构耦合到光纤探针表面。本文基于共价键结合原理,将3-巯丙基三甲氧基硅烷通过与锥形光纤探针表面的硅羟基形成共价键修饰在光纤上;同时,硅烷偶联剂末端的巯基与金或银纳米结构形成Au-S或Ag-S共价键,将金纳米粒子和银纳米立方体牢牢吸附到光纤探针表面。这种SERS光纤探针具有很高的稳定性(SERS信号相对标准偏差低于3%),对农残甲基对硫磷的敏感度达到10纳摩尔,对污染物的远程、便携式在线检测具有重要意义。     

一种用于现场快速检测的SERS基底的制备

利用化学自组装方法,首先在色谱玻璃小瓶的内壁吸附上一层PDDA阳离子聚电解质,然后通过静电吸附作用将带有负电荷的银纳米粒子组装到内壁;比较了不同色谱瓶作为吸附银纳米粒子的载体的优缺点;用紫外-可见吸收光谱监测吸附到玻璃瓶内壁的银纳米粒子的表面等离子体共振峰,跟踪银纳米粒子的组装情况;利用对-巯基苯胺作为探针分子研究了基底的表面增强拉曼散射(SERS)活性。结果表明：所制备的SERS小瓶基底具有良好的SERS活性,并且使用简单,保存时间长,适合SERS现场快速检测的需要。     

一种用表面增强拉曼光谱进行免疫检测的方法

一种结合表面增强拉曼(SERS)技术和纳米粒子标记技术,通过银增强来实现免疫检测的方法。将p-巯基苯甲酸(MBA)作为探针,固定在免疫金溶胶粒子表面形成纳米标记,其与被基底捕获抗原分子发生免疫识别。通过银增强技术,在"三明治"结构对探针进行拉曼检测。     

纳米粒子修饰硅胶整体柱的制备及其在柱表面增强拉曼光谱应用研究

通过溶胶-凝胶法以四甲氧基硅烷(TMOS)和甲基三甲氧基硅烷(MTMS)作为混合的前体,聚乙二醇(PEG)为致孔剂,制备了具有贯通孔道结构的双孔硅胶整体柱,采用3-巯基丙基三甲氧基硅烷(MTPMS)对硅胶整体柱表面进行巯基化修饰后,分别将金、 银纳米粒子组装在整体柱材料表面。 利用透射电子显微镜(TEM)、 紫外-可见吸收光谱(UV-Vis)、 扫描电子显微镜(SEM)对金、 银纳米粒子形貌、 吸收光谱及组装金、 银纳米粒子前后整体柱的形貌进行了表征。 以对巯基苯胺(PATP)为探针分子,分别采用波长为633和532 nm的激发光作为激发光源,研究金和银纳米粒子修饰的硅胶整体柱的在柱表面增强拉曼光谱(SERS)性能。 结果表明,该基底呈现出很强的SERS活性,结合整体柱的分离富集优势将在食品/环境领域现场痕量检测方面具有广泛的应用前景。     

银纳米粒子修饰三维碳纳米管阵列SERS实验

为了使表面增强拉曼散射(SERS)基底的三维聚焦体积内包含更多的“热点”,能吸附更多探针分子和金属纳米颗粒,以便获得更强的拉曼光谱信号,提出了银纳米粒子修饰垂直排列的碳纳米管阵列三维复合结构作为SERS基底,并对其进行了实验研究。利用化学气相沉积(CVD)方法制备了垂直排列的碳纳米管阵列;采用磁控溅射镀膜方法先在碳纳米管阵列上形成一层银膜,再通过设置不同的高温退火温度,使不同粒径的银纳米粒子沉积在垂直有序排列碳纳米管阵列的表面和外壁。SEM结果表明：在有序碳纳米管阵列的表面和外壁都均匀地负载了大量银纳米粒子,并且银纳米颗粒的粒径、形貌及颗粒间的间距随退火温度的不同而不同。采用罗丹明6G(R6G)分子作为探针分子,拉曼实验结果表明：R6G浓度越高,拉曼强度越强,但是R6G浓度的增加与拉曼强度增强并不呈线性变化;退火温度为450 ℃,银纳米颗粒平均粒径在100～120 nm左右,退火温度为400 ℃,银纳米颗粒平均粒径在70 nm左右,退火温度为450 ℃的拉曼信号强度优于退火温度400和350 ℃。     

银和去合金银-金纳米粒子的SERS活性研究

用乙二醇还原硝酸银,聚乙烯吡咯烷酮作表面活性剂合成了大量的银纳米颗粒。银纳米颗粒和HAuCl4发生置换反应后形成去合金银-金纳米粒子。以吡啶和SCN-作为探针分子研究了它们的SERS活性。结果表明,当探针分子吸附于银纳米颗粒和去合金银-金纳米粒子上时,探针分子的特征振动峰强度增强、频率发生位移。SERS可表征纳米粒子物理和化学性质的变化。     

银纳米立方体的合成及其SERS活性研究

用乙二醇还原硝酸银,以聚乙烯吡咯烷酮作表面活性剂合成了银纳米立方体晶粒,并以吡啶和SCN-作为探针分子初步研究了银纳米立方体晶粒组装体系的SERS活性。当探针分子吸附于银纳米立方体晶粒上时,吡啶和SCN-的谱峰强度明显增强,表明银纳米立方体晶粒可望作为SERS活性基底。通过研究探针分子的SERS强度与粒子尺度关系,也有望用于表征银纳米立方体晶粒的光学性质。     

银纳米阵列直径对SERS增强效果的影响

采用电化学沉积法分别在不同孔径的阳极氧化铝(AAO)模板上沉积一系列直径不同,排列规则的银纳米阵列。以对氨基苯甲酸(PABA)和三聚氰胺两种分子分别作为探针分子, 研究了银纳米阵列的直径大小对其表面增强拉曼散射(SERS)效果的影响。结果表明, 在波长为514.5 nm的激光激发下, 探针分子的SERS信号强度随银纳米阵列直径的改变而明显变化, 并在银纳米阵列直径约为53 nm时, SERS强度达到最大。利用电磁增强机制对此实验结果进行了分析和解释。     

基于金/银纳米三明治结构SERS特性的超灵敏前列腺特异性抗原检测

基于金/银纳米三明治结构的表面增强拉曼散射(SERS)特性, 实现了前列腺特异性抗原(PSA)高灵敏度免疫检测, 检测结果具有特异性。采用化学还原法制备金、银纳米粒子, 用4-巯基苯甲酸(4-MBA)及前列腺特异性抗体(Anti-PSA)链接金、银纳米粒子制备免疫探针, 在硅片表面原位生长金、银纳米粒子并链接Anti-PSA制备得到免疫基底。将免疫探针、免疫基底以及PSA组成三明治结构, 进行基于SERS特性的免疫检测。实验结果表明, 纳米银免疫探针与纳米银免疫基底组成的三明治结构具有最佳的检测效果, PSA的检测灵敏度低至1.8fg/mL(3.490吆^-18mol/L), 可应用于前列腺癌症的早期检测与诊断。     

氯离子对固定银纳米颗粒SERS活性的影响

通过在硅片上修饰聚乙烯吡咯烷酮(PVP)对银纳米粒子进行组装,得到均一的表面增强拉曼光谱(SERS)基底。借助于此基底,在水溶液环境中,以异烟酸(INA)和罗丹明6g(R6g)作为探测分子,研究了氯离子(Cl-)对SERS增强的影响。结果表明,对于不同的探针分子,Cl-对银颗粒SERS活性的影响存在选择性。对于INA分子,在溶液中没有Cl-的情况下,分子通过羧基以锐角吸附在银颗粒表面,具有良好的SERS谱。在加入Cl-后,由于竞争吸附,INA分子脱附,SERS信号消失。R6g分子在银颗粒表面没有特异吸附,Cl-的加入并没有影响其与银颗粒的作用状态,在加入Cl-后SERS光谱没有发生显著变化。     

多波长消荧光拉曼光谱仪的研制及应用研究

拉曼光谱技术作为探究分子、晶体及其结构特征的有力手段,具有快速、无损、样品用量小、无需前处理且适应性强等优点,已被广泛应用于食品安全、石油化工等领域。但在拉曼光谱应用中,常常受到荧光背景干扰,导致拉曼信号降低,严重的情况下拉曼信号甚至会淹没在荧光背景中。为解决拉曼技术在实际应用中荧光背景干扰的问题,从仪器角度出发,采用二色镜对多波长拉曼光谱进行光路耦合设计,研制了近红外拉曼光谱与移频差分拉曼复合一体的多波长消荧光拉曼光谱检测系统,其中近红外拉曼光谱采用1 064 nm激光光源设计,移频差分拉曼光谱选取784.5和785.5 nm两组激光光源进行时分复用,在移频差分拉曼光谱检测的同时,亦可获得两组单波长拉曼光谱数据。通过对比同步测试和分时逐次测试的强度及峰位稳定性,验证了多波长消荧光拉曼光谱仪的同步测试性能;选取了多种荧光背景强弱不同的样品,进行了单波长拉曼、近红外拉曼及移频差分拉曼光谱的对比分析。针对丙酮、乙腈等荧光背景较弱的样品,可采用单波长拉曼光谱对样品进行定量及定性分析;针对食用油、红色塑胶微粒等荧光背景与拉曼信号强度相当的样品,可采用近红外拉曼光谱对样品进行定量及定性分析;针对红酒、棕色塑胶微粒等荧光背景较强的样品,需结合近红外拉曼光谱和差分拉曼光谱对样品进行定性分析。研究表明：通过多波长消荧光拉曼光谱检测系统的研制,在常规单波长拉曼光谱技术的基础上,将两种抑制荧光干扰技术有机结合,有效扩充了应用领域及样品检测范围。     

Two‐dimensional standoff Raman measurements of distant samples

A scanning standoff Raman spectroscopy system has been developed to measure the molecular species of distant samples in two dimensions. Computer software is used to control the scanner pan and tilt angles, and Raman measurements are collected of the distant sample area in an x–y grid pattern. The Raman spectra at each grid point are measured and processed to obtain an image of the distant surface composition. The ability to provide interpolated images of distant molecular species is illustrated. Copyright © 2011 John Wiley & Sons, Ltd.     

拉曼光谱技术的应用及研究进展

本文简述了拉曼光谱产生的机理以及与红外光谱的区别,讨论了拉曼光谱在聚合物、生物分子、蛋白质和无机物等方面研究及应用,介绍了傅立叶变换拉曼、共焦显微拉曼、表面增强激光拉曼、固体光声拉曼光谱的原理及其应用以及拉曼光谱和其他检测手段的联用技术。     

复合输出镜（Nd,Ce）：YAG拉曼频移激光器研究

报道了由部分反射凹面镜和辅助平面镜构成的复合输出镜高压ＣＨ４气体（Ｎｄ，Ｃｅ）：ＹＡＧ拉曼频移激光器的理论和实验研究结果，在１０Ｊ的输入下，获得１２ｍＪ的拉曼激光输出，并计算的基频场基模光束参数。     

拉曼光谱技术在爆炸物检测中的应用

随着恐怖活动的蔓延,对爆炸物的检测和溯源变得越来越重要。拉曼光谱能够提供化合物的指纹图谱,是对物质定性分析的有力工具,具有无损、快速、准确度高等优点,近年来在爆炸物检测领域被广泛应用。本文介绍了共聚焦显微拉曼光谱、空间偏移拉曼光谱、表面增强拉曼光谱等拉曼光谱技术在爆炸物检测方面的应用及最新研究进展。     

A novel Raman optical activity instrument operating in the deep ultraviolet spectral region

Raman optical activity (ROA) has been exclusively observed in the visible (VIS) and near‐infrared (NIR) spectral regions to date. During the last few years, we have designed, constructed and tested the first ROA instrument, operating in the deep‐ultraviolet (DUV) spectral region employing 244‐nm excitation. This novel DUV ROA instrument is based on a backscattering geometry and incident circular polarization modulation (ICP); it makes use of a fast DUV imaging lens‐based spectrograph and specially designed DUV grade polarization optics. The performance of this instrument has been evaluated by analysing measured non‐resonant DUV ROA spectra of non‐absorbing enantiomeric liquid samples and by comparing these with corresponding ROA spectra recorded in the visible spectral region. Copyright © 2015 John Wiley & Sons, Ltd.     

高压下NaCl水溶液的Raman光谱不连续性的证据

在温度21 ℃和压力50～1 100 MPa范围内利用碳化硅压腔进行了10％的NaCl水溶液的Raman光谱的原位测量和研究。研究发现：溶液的Raman拟合谱峰在50～300 MPa压力范围内,随着压力的增加向低波数方向移动,在约300 MPa时达到最小值;在300～800 MPa压力范围内,压力的升高则导致谱峰向高波数方向移动,在约800 MPa时达到最大值;随着压力的进一步升高(＞800 MPa),谱峰又向低波数方向移动。类似地,拟合谱峰的峰面积比值和半高宽在压力约300和800 MPa时也发现了不连续现象。这表明高压下NaCl水溶液的内部结构是不连续的,溶液中的氢键(O—H…Cl-)发生了相应的变化,意味着溶液中出现了结构的重新排列,产生了较为复杂的结构构型。     

Stimulated Raman scattering and spontaneous Raman solitons in ammonia

In this study we report the first observation of spontaneous Raman solitons in stimulated Raman scattering (SRS) by the gas NH₃. The scattered radiation is called Stokes radiation. Raman solitons are of considerable interest, because their existence can be explained by quantum-mechanical fluctuations of the electromagnetic field in vacuum. We have observed spontaneous Raman solitons in a forward SRS configuration for two different molecular transitions of NH₃, the laser emissions at 58 μm and 72.6 μm wavelength. These are optically pumped by 10 μm CO₂-laser pulses with a duration of 100 ns and an energy of 150 mJ. Spontaneous Raman solitons are short spikes in the pump pulse which occur during its depletion. Their origin is the rapid π phase change of the Stokes seed. In contrast to other laboratories we have used single-pass cells. Thus, we have succeeded in observing multiple spontaneous Raman solitons during one pump pulse. Previous experiments with multi-pass cells never showed multiple solitons. Since multiple spontaneous Raman solitons have already been reported in an earlier experiment with a single-pass cell filled with hydrogen at high pressure, we conclude that such multiple Raman solitons can be observed mainly in this type of gas cell. Subsequently, we have performed statistical measurements on the delay time and the height of the spontaneous Raman solitons in the depleted pump pulse for the 58 μm-NH₃ emission. We have compared these statistics with theory and equivalent experimental results of other laboratories. They are in good agreement with the assumption that quantum-mechanical fluctuations are the origin of spontaneous Raman solitons. The most recent theories postulate that the origin of the formation of spontaneous Raman solitons can be explained by the rapid π phase change of the Stokes seed as well as that of the laser or polarization wave. Therefore, we have determined the phase of the spontaneous Raman solitons relative to the depleted pump pulse. Although, such changes of sign of the relative phase have already been observed in an earlier SRS experiment with hydrogen at high pressure, we did not detect any in our experiment. Therefore, we conclude that in this experiment the π phase change occurs in the Stokes or polarization wave.     

Raman Scattering Intensities of the NO2 Symmetric Stretching Vibration Band of Some Aromatic Nitrocompounds (II)

The Raman scattering intensities of the NO₂ symmetric stretching vibration band were investigated experimentally for some para and meta substituted nitrobenzenes. The excitation profiles obtained with the six excitation wavelengths from 457.9 to 514.5 nm were presented. The results were examined in terms of the Albrecht-Hutley's theory, and the electronic states involved in the preresonance Raman intensity enhancement were suggested.     

Identification of Explosive Substances Through Improved Signals Obtained by a Portable Raman Spectrometer

The development of devices to detect explosive substances in situ with characteristics such as easy portability, simple operation, and quick response is of high interest nowadays. Raman spectroscopy meets most of these requirements, allowing for the identification of volume and trace amounts of an unknown substance. In this paper we report the characterization of explosive substances such as ANFO and pentolite, both in their pure forms as well as mixed with other substances, such as sugar and sodium hydrogen carbonate, using a portable Raman Enwave Optronics EZRaman-model M, whose signal is sent and received by a head coupled to an optical fiber. The obtained spectra have been validated by comparison with those obtained by a conventional Raman spectrometer with high resolution. We discuss the advantage of using miniaturized laptops running with a 785-nm laser, making a correction of the signal response to obtain optimized spectral fingerprints with minimum noise, in order to design an autocalibrated, easily portable device that performs the function of identification of the mentioned substances.