层析滤纸拉曼光谱特性研究

为了研究层析滤纸在表面增强拉曼光谱和层析技术联用中的影响。在785 nm激发波长下分别测试了层析滤纸, 涂布银胶后层析滤纸的拉曼特征谱, 以及氧化乐果在层析滤纸上的拉曼光谱和表面增强拉曼光谱(SERS)。结果表明, 层析滤纸在800~1500 cm-1光谱区域具有丰富的拉曼特征峰, 分析认为主要来源于纤维素, 并对其进行了归属; 涂布银胶后, 由于银颗粒的作用, 层析滤纸拉曼强度整体降低, 并发生特征峰相对强度的变化; 同时, 氧化乐果在层析滤纸上的SERS谱也表明涂布银胶能够有效抑制层析滤纸拉曼特征峰, 增强待测物质拉曼强度, 但在800~1500 cm-1光谱区域仍需考虑层析滤纸的影响。     

白术煎剂表面增强拉曼光谱分析

测试分析了白术煎剂及其在银胶中的拉曼光谱,并对其进行初步谱峰归属。白术煎剂表面增强拉曼光谱在396,548,617,730,955和1 327 cm-1处,出现6个明显的拉曼信号。测试了白术煎剂和白术煎剂-银胶混合体系的紫外-可见吸收光谱,该吸收光谱在长波区出现新共振吸收峰(999 nm处),进而研究了白术煎剂在银溶胶上的吸附特性及其表面增强机理。结果表明,表面增强拉曼光谱可能为白术煎剂或其他中药煎剂提供一种准确、直接、快速的检测方法。     

氨基酸在银胶溶液中的表面增强拉曼效应

文章报道了通过制备合适的银胶盐纳米溶液 ,得到的甘氨酸、缬氨酸和赖氨酸在银胶溶液中的表面增强拉曼光谱。低波数 2 38cm-1谱带的出现 ,表明氨基酸分子已与银表面产生明显吸附。在所得SERS图谱中 ,表征C—C基团的 90 0～ 930cm-1谱带、表征NH2 基团的 110 0cm-1左右谱带和表征COO-基团的14 0 0cm-1附近的谱带振动都得到显著加强 ,其原因主要是通过羧基基团及氨基基团与银粒子表面产生吸附 ,增强机制属于化学增强 ,为短程效应。本实验中 ,当银胶溶液 pH值降低时 ,对拉曼散射的增强效果影响不大。     

家蚕微粒子虫表面增强拉曼光谱研究

本文报导并分析了家蚕微粒子虫(Nosema bombycis Naegeli,缩写为NbN)孢子在PH4.0条件下的表面增强拉曼光谱(SERS),在常规的实验条件下未得到NbN的一般拉曼谱,同时也未获得其它PH条件下的表面增强拉曼谱。对获得的NbN的SERS分析表明:NbN孢子通过S原子,COO~-和NH_2基团被吸附到银胶表面上,Tyr、Trp残基侧链靠近银表面,以Tyr残基侧链的振动增强效应最显著。当NbN孢子吸附在银胶表面时,NbN孢子中的C—C—S—S—C—C链为扭曲—扭曲—反式结构。     

基于密度泛函的伪麻黄碱拉曼光谱性质研究

研究伪麻黄碱的拉曼光谱和吸附在纳米银基底上的表面增强拉曼光谱(SERS),利用密度泛函理论B3LYP/6-311G++(d, p)方法对伪麻黄碱分子进行了计算,得到了分子构型信息和理论拉曼光谱,用Gaussview软件对分子振动模式进行了全面的归属,在伪麻黄碱的表面增强拉曼光谱中,采用了自组装方法获得了团簇银纳米表面增强基底,实现了很好的增强效应.实验结果表明：伪麻黄碱的拉曼光谱计算结果和实验结果基本一致,理论计算为伪麻黄碱分子振动峰位的归属提供了重要的依据,伪麻黄碱分子与银纳米表面化学吸附,苯环垂直于纳米基底表面,研究结果为伪麻黄碱的拉曼光谱检验分析提供了理论依据,也为苯丙胺类毒品的光谱分析研究提供了参考.     

维生素K3的表面增强拉曼光谱研究

首次报道了维生素K3 (VK3 )分子的常规拉曼光谱 (NRS)及该分子在活性衬底银镜上的表面增强拉曼散射 (SERS) ,并对它的拉曼特征谱带进行了初步的指认和归属。通过对比VK3 的常规拉曼光谱和SERS谱 ,发现VK3 分子吸附在银表面后拉曼散射强度被大大增强了。另外 ,VK3 的羰基与银粒子发生电荷转移后形成负离子自由基 ,碳氧双键打开。受VK3 分子吸附在银镜表面的影响 ,萘环结构发生了很大的扰动 ,导致一些拉曼特征峰产生位移 ,环变形振动对应的拉曼散射强度得到了增强。这些研究结果为SERS技术今后对VK3进行药物检测以及痕量分析方面的应用提供了依据。     

银胶和银岛膜上胸腺嘧啶的表面增强拉曼光谱对比研究

利用表面增强拉曼光谱对胸腺嘧啶在银胶和银岛膜上的吸附状态进行了对比研究.光谱分析表明,胸腺嘧啶吸附在银胶和银岛膜表面后其分子结构发生了互变异构,由原来的酮式结构变成了烯醇式结构.在银胶和银岛膜表面胸腺嘧啶主要以N(3)去质子化异构体的形式存在.胸腺嘧啶通过O(7)和N(3)倾斜地吸附在银胶颗粒表面,通过O(8)和N(3...     

菜粉蝶颗粒体病毒包涵体在银胶中的表面增强拉曼光谱研究

本文讨论了菜粉蝶(preris rtpae)颗粒体病毒(简称 PrGV )包涵体在银胶中的表面增强拉曼光谱。PrGV 包涵体的 SERS 谱与其 RS 谱之间存在一定对应关系。PrGV 包涵体蛋白分子通过羧基和氨基基团吸附于银粒子表面,并构成阴离子形式(NU_2RCOO~-)存在于溶液中。PrGV 在银胶中的表面增强的增强机制属于短程作用。PrGV 包涵体与银胶表面的吸附主要是化学吸附。     

一种新型基底上右旋肉碱的表面增强拉曼光谱研究

在聚乙烯吡咯烷酮(PVP)存在下,用多元醇还原硝酸银,Cu(NO₃)₂作为保护剂,快速有效的合成大量银纳米线,并优化了反应条件,得到结构均一、分散性较好的银纳米线。以罗丹明B为探针分子检测了该银纳米基底的表面增强效应,结果表明该基底对罗丹明B的表面增强效果明显,其表面增强因子可达6.4×105。文中利用这种基底得到了右旋肉碱的表面增强拉曼光谱(SERS),与其固体常规拉曼光谱(NRS)和10-3 mol·L-1水溶液的拉曼光谱对比,并对各自的峰位进行了归属。右旋肉碱固体在3 100～2800和1 700～200 cm-1处有明显拉曼振动峰,在右旋肉碱的表面增强拉曼光谱中,1700～200 cm-1处的峰得到了明显的增强。经分析,右旋肉碱分子与银纳米基底呈180°。本文还用合成的纳米银基底得到了不同浓度右旋肉碱溶液的表面增强拉曼光谱,其最低检测浓度为10-6 mol·L-1。右旋肉碱是一种重要的心血管药物,本文为其研究提供了较全面的拉曼光谱信息,为右旋肉碱的快速、特征、痕量监测提供了有力依据,也为进一步研究右旋肉碱的药理学提供了重要参考。     

维生素A酸在银溶胶液中的表面增强拉曼散射光谱

将水中不溶的药物维生素A酸(VAA)溶于氯仿中,然后与银溶胶液混合,振摇,取静置分层后的上层溶胶液测定表面增强拉曼光谱,氯仿在银溶胶中无表面增强效应,不干扰维生素A酸的测定。与固体粉末拉曼光谱相比较,对光谱峰归属进行了解释。通过分析CO伸缩振动带和ν(COO)振动峰明显增强的现象,讨论了维生素A酸分子在银颗粒表面可能的吸附取向,并推断维生素A酸在银表面的吸附发生在COO-基团。以维生素A酸表面增强拉曼光谱在1583cm-1处的峰强度对浓度进行线性回归,求得线性回归方程Y=10×108+95585,在10×10-6～50×10-5mol·L-1范围呈良好的线性关系,最小检测限为10×10-7mol·L-1。结果表明,维生素A酸表面增强拉曼光谱峰数量少,灵敏度高,是定量分析痕量维生素A酸的很好方法。     

Raman lasing and cascaded coherent anti-Stokes Raman scattering of a two-phonon Raman band

Raman lasing of a two-phonon Raman band in the anti-Stokes side is demonstrated. Two femtosecond light pulses with identical wavelengths are irradiated onto a SrTiO3 crystal in a cross-beam configuration. Under low excitation power, several wave-mixing signals with identical wavelengths are emitted. When the power exceeds a critical value, cascaded coherent anti-Stokes Raman scattering (CARS) signals are emitted, the frequency step of which is coincident with that of the strongest two-phonon Raman band of 2TO2.     

利用拉曼孤子实现宽带拉曼脉冲压缩

从拉曼散射方程的出发,研究了利用拉曼孤子实现宽带拉曼脉冲压缩的机制,发现孤子脉冲的宽度随拉曼增益的增加减小,并与 运光的脉冲形状及相位结构有关。实验中利用ＸｅＣｌ激光／Ｈ２系统初步实现了５０％的压缩率,并将实验结果与理论进行了比较。     

Coherent anti‐Stokes Raman scattering in Raman lasers and Raman wavelength converters

In this paper recent research progress on the use of Coherent Anti‐Stokes Raman Scattering (CARS) in Raman lasers and Raman wavelength converters is reviewed. The latest insights in the physical nature and behavior of CARS are addressed, and the recent performance breakthroughs in CARS‐based Raman wavelength conversion are discussed. Based on the new findings regarding the behavior of CARS, a physical explanation for apparent inconsistencies in various experimental observations of Raman wavelength conversion is provided. To conclude it is shown that these recent insights also pave the way to the development of a novel CARS‐based mechanism for reducing the heat dissipation in Raman lasers.     

拉曼增益系数可分离光纤中的受激拉曼散射

给出了拉曼增益系数分离光纤的定义,在考虑了N个单色光之间的两两受激拉曼散射,得到了这种光纤中单向传输的N个不同的单色光之间的受激拉曼散射（SRS）稳态耦合波方程的解析解。它适用于各单色光功率任意大小、光频率分布不均匀时的一般情况。这一结果可应用于光纤通信系统、拉曼光纤放大器和拉曼光纤激光器的设计与分析。最后把解析解与数值解进行了比较,两者取得了很好的一致。     

麻黄素和左旋咪唑显微拉曼测试分析

在可见光激发下，利用显微拉曼技术得到了黄素和左旋旋咪唑的拉曼谱，并将它们的拉曼谱和甲基安非地明做了对比分析，麻黄素和甲基安非他明同属单取代苯，其分子结构十分相似，由于取代基的成分不同一样，因而拉曼谱中一些峰的相对强度和位置发生了变化。左旋咪唑由于取代基上为咪唑亚塞唑，其拉曼谱中主要谱线位置和强度明显不同于麻醉黄素和甲基安非他明。实验结果表明，利用显微拉曼技术在短时间内，对致幻药物进行准确快速的检测分析，将这一技术应用于运动比赛中，有助于对参赛人员服用违禁药物的检测和分析。     

痕迹走私海洛因显微拉曼测试分析

利用显微拉曼技术对手指沾有微量毒品--走私海洛因做了测试分析，在可见光514.5nm激发下，低浓度的走私海洛因具有很强的荧光，通过对样品表面的分析，得到了高质量的海洛因拉曼散射谱。研究表明选取样品表面合适测试点和控制激光功率对减小走私海洛因拉曼散射谱的荧光有明显的作用。     

用于光纤拉曼放大器抽运源的单级光纤拉曼激光器

抽运光源是光纤拉曼放大器应用于密集波分复用系统的关键技术,设计了一种紧凑型的808nm激光二极管抽运的基于钒酸钇（Nd^3＋：YVO4）晶体1342nm固体激光器模块,提出利用上述1342nm固体激光器抽运基于光纤光栅的单级全光纤型拉曼谐振器获得1．4μm激光输出的光纤拉曼激光器,分析了固体激光器的阈值特性、性能优化方法和单级光纤拉曼谐振器的设计方法。上述1342nm固体激光器模块在抽运功率2W时获得了最大655mW的激光输出功率和42．6％的斜率效率,单级拉曼谐振器的1342nm到1．4μm光功率转换斜率效率达75％,在1425nm、1438nm、1455nm和1490nm处的输出功率达到300mW以上。最后给出基于1．4μm光纤拉曼激光器抽运的宽带平坦放大的光纤拉曼放大器的结构参量和性能测试结果。     

Raman response function and Raman fraction of phosphosilicate fibers

The Raman response function and Raman nonlinear index of phosphosilicate fibers are calculated for several P₂O₅ concentrations. The nonlinear index of phosphosilicate fiber is estimated by using the Boling formula, and it is used to calculate the Raman fraction of the nonlinear index. On the other hand, the Raman response function of the phosphosilicate fibers is fitted to a superposition of six phase-shifted under-damped functions in order to use it in the numerical simulation of ultra-short pulse propagation. We show through numerical simulations that phosphosilicate fibers are a suitable medium to observe a scaling up of the Raman self-frequency shift when compared to silica fibers.     

Raman susceptibility measurements and stimulated Raman effect in KDP

The propagation constant of the stimulated Raman process and Raman susceptibility measurements in KDP are reported. The stimulated Raman scattering due to 915 cm^-1 and 93 cm^-1 vibration in KDP has been experimentally observed.     

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.