(NH_2CH_2COOH)_2CdCl_2晶体的拉曼光谱的研究

（ＮＨ２ＣＨ２ＣＯＯＨ）２ＣｄＣｌ２晶体的拉曼光谱的研究刘建军吴粤郑吉民扈士芬蓝国祥（南开大学天津３０００７１）ＲａｍａｎＳｐｅｃｔｒａｏｆ（ＮＨ２ＣＨ２ＣＯＯＨ）２ＣｄＣｌ２ＣｒｙｓｔａｌｓＬｉｕＪｉａｎｊｕｎ，ＷｕＹｕｅ，ＺｈｅｎｇＪｉｍｉｎ，Ｈ...     

纳米三氧化二铬的拉曼散射

纳米三氧化二铬的拉曼散射左健冯建平许存义（中国科学技术大学结构分析开放实验室安徽合肥２３００２６）吴若（江西师范大学物理系江西南昌３３００２７）ＲａｍａｎＳｃａｔｅｒｉｎｇｏｆＮａｎｏｓｃａｌｅＣｈｒｏｍｉｃＯｘｉｄｅｓＺｕｏＪｉａｎ，ＦｅｎｇＪｉａ...     

掺Ce的Y－Ba－Cu－O体系成相的拉曼光谱分析

掺Ｃｅ的Ｙ－Ｂａ－Ｃｕ－Ｏ体系成相的拉曼光谱分析许存义，左健，王跃（中国科学技术大学结构分析开放研究实验室合肥２３００２６）ＳｔｕｄｙｏｎＴｈｅＲａｍａｎＳｐｅｃｔｒｕｍｏｆＣｅ－ｄｏｐｅｄＹ－Ｂａ－Ｃｕ－ＯＳｙｓｔｅｍ￥ＣｕｎｙｉＸｕ；ＪｉａｎＺｕ...     

TCNQ/C_(60)及MB-PPV/C_(60)等组合薄膜的拉曼光谱

ＴＣＮＱ／Ｃ６０及ＭＢ┐ＰＰＶ／Ｃ６０等组合薄膜的拉曼光谱钱江单福凯钱士雄魏彦峰黄大鸣华中一（复旦大学物理系上海２００４３３）ＲａｍａｎＳｐｅｃｔｒａｏｆＴＣＮＱ／Ｃ６０ａｎｄＭＢ┐ＰＰＶ／Ｃ６０ＣｏｍｂｉｎａｔｉｏｎＦｉｌｍｓＱｉａｎＪｉａｎｇ，Ｓ...     

PYAB单晶的拉曼光谱

ＰＹＡＢ单晶的拉曼光谱王继扬潘恒富（山东大学晶体材料研究所济南２５０１００）李丽霞（山东大学环境工程系济南２５０１００）ＶｉｂｒａｔｉｏｎａｌＳｐｅｃｔｒｕｍｏｆＰＹＡＢＳｉｎｇｌｅＣｒｙｓｔａｌＷａｎｇＪｉｙａｎｇ，ＰａｎＨｅｎｆｕ（Ｉｎｓｔｉｔｕ...     

腐植酸物质的表面增强拉曼散射

腐植酸物质的表面增强拉曼散射Ｅ．Ｊ．Ｌｉａｎｇ（梁二军）１，３，Ｙ．Ｈ．Ｙａｎｇ（杨育晖）３，Ｗ．Ｋｉｅｆｅｒ３１．郑州大学物理工程学院郑州４５００５２２．中国科学院化学研究所北京１０００８０３．ＩｎｓｔｉｔｕｔｆｕｅｒＰｈｙｓｉｋａｌｉｓｃｈｅＣｈ...     

四—（对—羟基苯基）卟啉在水／三氟乙酸溶液中J—聚集的光谱研究

本文研究了四－（对－羰基苯基）卟啉（ＴＣＰＰ）在Ｈ２Ｏ／ＣＦ３ＣＯＯＨ、Ｈ２Ｏ／ＣＣＩ３ＣＯＨ和Ｈ２Ｏ／ＣＨ３ＣＯＯＨ溶液中的ＵＶ－Ｖｉｓ吸收光谱、荧光光谱和拉曼光谱。实验表明,ＴＣＰＰ在Ｈ２Ｏ／ＣＨ３ＣＯＯＨ和Ｈ２Ｏ／ＣＣＩ３ＣＯＯＨ溶液中以分子态的Ｎ－质子化卟啉Ｈ８ＴＣＰＰ＾２＋存在,而在Ｈ２Ｏ／ＣＦ３ＣＯＯＨ中则形成Ｈ８ＴＣＰＰ＾２＋的Ｊ－聚集体。Ｊ－聚集体显示,ＵＶ－Ｖｉｓ吸收光谱和荧光光     

直接键连原子间的NMR偶合常数的自然杂化轨道研究V.~(13)C-~(13)C和~(13)C-~(31)P核自旋偶合常数~1J_(CC)和~1J_(CP)

在前文工作的基础上，结合ＭＮＤＯ／ＥＨＭＯ分子轨道方法和自然杂化轨道方法，具体计算了ＣＣ键和ＣＰ键的核自旋偶合常数．计算结果表明，１ＪＣＣ和１ＪＣＰ主要由成键原子的轨道杂化作用和键极性这两种结构因素所决定．为从简单价键理论角度解释和计算１ＪＣＣ和１ＪＣＰ值提供了简便直观的方法．     

共振拉曼光谱研究卟啉二酸H_4~(2+)TSPP的J-聚焦

用共振拉曼光谱和ＵＶ Ｖｉｓ吸收光谱考察了离子强度对四一（对一磺酸基）苯基卟啉二酸（Ｈ２＋４ＴＳＰＰ）Ｊ 聚集体形成的影响。实验表明加入少量的ＮａＣｌＯ４有助于聚集体的形成,而Ｎａ ＣｌＯ４的浓度过高则倾向于形成单体。ＮａＣｌＯ４的加入不改变聚集体中分子的构型和排列方式,但高浓度的ＮａＣｌＯ４可能在聚集体中引入某种缺陷,使激子态发生局域化。我们还得到了具有宏观尺寸的纤维状Ｈ２＋４ＴＳＰＰ沉淀,并研究了其固体显微拉曼谱。     

空气对C60薄膜拉曼谱的影响

采用拉曼光谱方法和光学二次谐波方法，观察蒸镀在石英玻璃上的Ｃ６０薄膜在空气中的变化，根据实验中观察的Ｃ６０薄膜１４６９ｃｍ＾－１拉曼谱的演变情况，结合二次谐波的测量结果，初步推断Ｃ６０分子发生了聚合反应和氧化反应。     

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。     

用光纤回路镜组成运转在1240 nm的新型串级光纤拉曼激光器

由光纤回路镜组成的新型串级光纤拉曼激光器,用1064nm作为抽运源,光纤拉曼激光运转于第三级斯托克斯串级拉曼波段,输出波长为1240nm。在光纤回路镜的性能和光纤参数还不够完善的条件下,1240nm输出功率为300mW,光－光转换效率约为25％。     

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。     

拉曼光谱编码的荧光液相生物芯片检测系统研究

随着医疗诊断需求的增加,生物分子检测技术越来越受到人们的重视,液相生物芯片技术作为一种高通量,多通道的分子检测手段在近几年得到了飞速发展。通过层层自组装方法制备以微片为载体的拉曼光谱编码液相生物芯片,并利用自行搭建的一套高灵敏度、高分辨率的光学系统,实现对液相生物芯片的定性与定量分析。光学系统由拉曼光谱检测系统与荧光显微成像系统耦合而成。在拉曼光谱检测系统中激光器发射出785 nm波长的激光,通过二向色镜,带反反射镜与物镜汇聚到样品上,样品产生的拉曼散射光,经物镜,带反反射镜,二向色镜与拉曼滤波片,最后通过凹透镜聚焦到光谱仪的狭缝上,光谱仪色散实现在线阵CCD上拉曼光谱的获取。荧光显微成像系统应用光学成像原理,通过调节凹透镜与405 nm的激发光之间的距离,使激发光通过物镜均匀的照射到样品之上,样品激发出的荧光,通过物镜,带反反射镜,二向色镜,滤波片与相应的凹透镜,最后成像到面阵CCD上。改进传统便携式拉曼光谱检测系统光路并选用相应波段的带反反射镜与焦距20倍的物镜完成拉曼光谱检测系统与荧光显微成像系统的耦合。为了减少两路系统之间的相互影响选用合适的二向色镜以及滤波片,在提高耦合系统获取数据的准确性中有着重要的作用。该系统通过对反应之后的液相生物芯片进行拉曼光谱检测,以完成对每个编码玻片的定性识别,即解码;同时激发反应后液相生物芯片的荧光并采集荧光强度图,根据每个解码玻片上的荧光强度值完成对目标检测物的定量分析。区别于传统荧光编码液相生物芯片, 拉曼光谱编码具有稳定性更强,光谱分辨率更高等优点。该光学系统集拉曼光谱检测系统与荧光显微成像系统于一体,解决了目前未有基于拉曼编码的液相生物芯片的检测系统的问题,并且可同时对多种目标物进行识别和定量分析,提升了实验结果的准确性。     

Simultaneous Double-Color Continuous Wave Raman Fiber Laser at 1239 nm and 1484 nm Using Phosphosilicate Fiber

Simultaneous double-color high-power continuous wave (CW) Raman fiber laser at 1239 nm and 1484 nm is demonstrated which uses CW 8.4 W Yb-doped double-clad fiber laser at 1064 nm as a pump, 1 km phosphosilicate fiber, and cascaded cavities consisting of two pairs of fiber Bragg grating (FBG) mirrors. Maximum output powers are 0.65 W at 1239 nm and 0.97 W at 1484 nm with a 50%/50% output mirror reflectivity pair, and 0.37 W at 1239 nm and 1.06 W at 1484 nm with a 75.5%/50% pair. The output characteristics of this laser for different FBG mirror reflectivities are reported.     

579 nm外腔式拉曼激光器传输耦合方程的数值计算

 为了提高以KGd(WO4)2晶体为拉曼介质的外腔式拉曼激光器的输出功率和转化效率,采用面积求和法编制matlab计算程序,对该激光器的传输耦合方程进行数值求解。计算得到了一至三阶斯托克斯光输出光强随时间的变化规律和受激拉曼散射的弛豫振荡过程。得出：拉曼谐振腔输出耦合镜对一阶斯托克斯光的反射率越高,拉曼谐振腔内的一阶斯托克斯光功率密度就越高,越有利于泵浦光向二阶斯托克斯光的转换。     

Passive signal enhancement in spatially offset Raman spectroscopy

We demonstrate experimentally, for the first time, the feasibility of enhancing signals in Spatially Offset Raman Spectroscopy (SORS) using a dielectric bandpass filter, building on our earlier experimental work on the enhancement of transmission Raman signals. The method is shown to lead to the enhancement of both the surface and subsurface Raman layer signal improving the signal‐to‐noise ratio of Raman spectra from the deep areas of samples, thus enhancing the technique's sensitivity and penetration depth. The filter is placed over the laser illumination zone, on the sample surface acting as a ‘unidirectional’ mirror transmitting the collimated laser beam on one side and reflecting photons escaping from the sample back into it. This enhances the degree of coupling of laser radiation into the medium and associated generated Raman signal. The feasibility study was performed on a two‐layer sample with the second layer located at the limit of the penetration depth of the method for this sample. The sample consisted of a 2.2‐mm over‐layer of a thinned paracetamol tablet followed by a 2‐mm layer of trans‐stilbene powder. The Raman signal was collected from a spatially offset region through a hole fabricated within the filter. The experiments demonstrate the presence of an enhancement of the Raman signal from both the layers by a factor of 4.4–4.5 and the improved signal‐to‐noise ratio of sublayer signal by a factor of 2.2, in agreement with photon shot noise dominated signal. Copyright © 2008 John Wiley & Sons, Ltd.     

Numerical optimization of the extracavity Raman laser with barium nitrate crystal

The radiation transfer equations of the extracavity Raman laser including up to the third Stokes beams and backward Raman scattering terms were deduced in detail from the wave equation and material equations of stimulated Raman scattering. The radiation transfer equations were solved numerically to optimize the performance of the extracavity Raman lasers with barium nitrate crystal as the nonlinear medium. The optimum reflectivity of the output coupler at the first Stokes was figured out numerically to achieve the maximum conversion efficiency of the first Stokes, and found to be closely related to the pump pulse duration, peak intensity of the pump pulse, and Raman crystal length. With the resonator mirrors highly reflective at the first Stokes, the highest conversion efficiency of the second Stokes was obtained when the input mirror was highly reflective at second Stokes, whereas the output coupler was highly transmissive at the second Stokes. It was found that too high intracavity intensity of the second Stokes would impede the efficient energy extraction from the pump pulse to the first Stokes, and consequently, limit the conversion efficiency of the second Stokes.     

Output Characteristics of High-Power Continuous Wave Raman Fiber Laser at 1239 nm Using Phosphosilicate Fiber

A high-power singlemode Raman fiber laser (RFL) with maximum output power of 4.11 W and maximum power conversion efficiency of 47.40% at 1239 nm is realized using continuous wave 8.4 W Yb-doped double-clad fiber laser as a pump, 700 m phosphosilicate fiber, and a Raman cavity formed by a pair of fiber Bragg grating mirrors at 1239 nm. The output characteristics of the RFL at 1239 nm for different fiber lengths and output mirror reflectance are reported. Theoretical simulation is done to numerically optimize for fiber length and output coupler reflectivity to obtain maximum first Stokes power.     

Normal incidence Raman scattering enhancement in double-cavity microresonators

We report on the observation of huge enhancements of the Raman scattering efficiency at quasi-backscattering due to double optical resonances in a microcavity. The structure, based on a double-cavity configuration separated by a central mirror, was specifically designed and grown by molecular beam epitaxy to achieve a large splitting, close to the energy of the LO phonon of GaAs, between the two confined photon modes.