胶原蛋白温度效应的Raman光谱研究

在不同温度下对Ⅰ型胶原蛋白进行了拉曼光谱测定。结果表明：随温度的升高，多数谱线向低波数移动，但CH2的变形振动谱线1302cm^-1向高波数移动，苯丙氨酸的特征振动谱线1003cm^-1的波数基本保持不变。同时还给出了拉曼谱线强度随温度的变化关系，得到了0，40，68，90℃四个变性峰，其中40，68℃的峰与DSC(差示扫描量热法)和SHG(二次谐波法)的测量结果一致，0℃的峰为冰冻相变，90℃的变性峰为胶原的二级结构被破坏所致。当温度达到150℃时，谱线强度显著降低，大部分谱线消失，胶原的一级结构遭到破坏。实验还发现胶原纤维在低温区具有较好的复性特性。     

乳腺癌病人单个细胞的Raman光谱

给出了乳腺癌病人正常乳腺细胞与癌细胞的拉曼光谱。从实验谱线中得到：癌变细胞的拉曼谱整体变弱, 就相对强度而言, DNA的2个磷酸根骨架峰782,1 084 cm-1和脱氧核糖-磷酸振动峰1 155及1 262 cm-1拉曼谱线明显的减少; 表征A型(DNA)构像的特征峰812 cm-1及谱线979,668 cm-1消失, 并有新峰1 175 cm-1出现, 905 cm-1的谱线增强并有6 cm-1的红移, 这说明DNA的磷酸根骨架有一定的断裂; 从而导致癌细胞的分裂繁殖失去有效的控制。在癌变组织细胞的拉曼谱中还发现了很强的一类与钙硬化密切相关的特征峰960 cm-1; 通过这些特征拉曼谱线的变化, 为癌症的诊断和治疗提供了有力的实验依据。     

温度对鱼鳞胶原蛋白二级结构的影响

从草鱼鱼鳞中提取酶溶性胶原蛋白(PSC),通过SDS-PAGE电泳分析为典型Ⅰ型胶原蛋白且达到电泳纯。在此基础上利用傅里叶变换红外光谱(FTIR)、拉曼光谱(Raman)和圆二色谱(CD)研究了温度对鱼鳞胶原蛋白二级结构的影响。FTIR分析表明：鱼鳞胶原蛋白具有典型的胶原蛋白特征吸收带,酰胺Ⅰ、酰胺Ⅱ和酰胺Ⅲ带的特征吸收频率分别出现在1658,1552和1238cm-1处。随温度升高,酰胺A和酰胺B峰位向低波数移动,1658cm-1处吸收峰裂解成多个吸收峰;1552cm-1处的吸收峰在35℃微略红移,随后发生明显蓝移;1238cm-1处吸收峰随温度升高向低波数移动。在拉曼光谱中,胶原蛋白的酰胺Ⅰ、酰胺Ⅱ和酰胺Ⅲ带的特征吸收频率分别出现在1669,1557和1245cm-1处,都较红外光谱的波数高;此外,921和855cm-1处脯氨酸的特征谱峰在拉曼光谱中体现出来。圆二色谱分析表明,胶原蛋白溶液在221.6和204.4nm分别有一正、负峰,具有典型胶原蛋白三螺旋结构的特征圆二色谱峰型。胶原蛋白冻干品的FTIR光谱和Raman谱线大都在35～60℃时发生波数和强度改变,而胶原蛋白乙酸溶液的CD谱线在20～35℃之间发生剧烈改变。由此可以判断胶原蛋白在固态和溶液状态下,变性温度存在一定差异,胶原蛋白冻干品比其乙酸溶液更稳定。     

LiB3O5晶体高温拉曼光谱研究

研究了LiB3 O5晶体在不同温度下(在300-1173 K的温度范围)的拉曼光谱,分析了LBO晶体结构随温度变化的规律.随着温度的升高,LBO晶体的拉曼光谱谱峰都不同程度地向低波数方向移动,也存在不同程度的展宽,同时强度减弱.发现晶体在1100 K存在明显相变,与LBO晶体的相图给出的1107 K的相变温度基本相符.     

高压下橄榄石的激光拉曼光谱研究

本文以实验为基础,给出了石英及橄榄石的拉曼谱图,利用不同压力点石英的拉曼位移公式计算了不同压力点的压力值;由橄榄石拉曼谱图得到了橄榄石拉曼特征峰随压力的变化情况:随压力的升高,橄榄石的拉曼特征峰向高波数方向偏移,两个拉曼峰之间的波数差减小,半峰宽增大,并且橄榄石的拉曼特征峰波数随压力的变化不是线性的。     

磷酸钠结构的高温拉曼光谱研究

用高温拉曼光谱仪测定了固态和熔融态磷酸钠(Na3PO4)晶体的光谱,分析了磷酸钠晶体的结构及其随温度的变化。通过对从常温谱到高温谱的解析,得出主峰波数随温度的变化及主峰半高宽的变化,可以观察到在600 K附近及1773 K有两个相变产生。此外,磷酸钠晶体的相关高温DSC检测分析,也和拉曼谱中发现的两个相变符合。量子化学理论计算同时对该体系的P-O键振动和平均键长进行了模拟,随着键长的增加,对应的振动频率会降低。还确认了磷酸钠Raman光谱中各个峰的归属,938 cm-1波数处的峰属于(PO4)3-中P-O键的对称伸缩振动,是Na3PO4的特征峰,425及580 cm-1处峰属于磷氧四面体的弯曲振动。     

KTN晶体及其熔体结构的高温拉曼光谱研究

测量并研究了不同温度(室温—1573 K)范围内KTN晶体的拉曼光谱及其熔体的高温拉曼光谱,分析了KTN晶体结构随温度变化的规律及其熔体的结构特征.随着温度的升高,KTN晶体的拉曼光谱谱峰都不同程度地向低波数方向移动,同时存在不同程度的展宽,并伴随强度的减弱.观察并解释了温度353 K附近KTN晶体样品的四方—立方转相现象.研究了KTN晶体拉曼光谱中538cm^-1,585cm^-1,835cm^-1和877cm^-1谱峰及其 关键词： 高温拉曼光谱 熔体 KTN晶体     

人血单个红细胞的共振拉曼光谱研究

给出了人血单个红细胞在不同激发光源下的共振拉曼光谱。从实验谱中得到 ,构象不灵敏的苯丙氨酸的单取代基环的伸缩振动谱线 10 0 2cm-1和吡咯环的CN呼吸振动谱带中 16 2 0cm-1的谱线 ,对 782nm激发光源共振较强 ,呈现出强度大而半高宽小的尖锐谱线 ;而在 5 14nm激发光源下 ,该两条谱线较弱。其他谱线 ,高波数段 (大于 135 0cm-1) ,在 5 14nm激发光源下 ,谱线强度大且清晰 ;低波数段 (小于 135 0cm-1) ,对应 782nm激发光源的拉曼谱线强而明显。同时还给出了同一激光光源下 ,取血后不同时间单个红细胞的拉曼光谱。发现对 782nm激发光源 ,除 16 0 1cm-1谱线强度减小外 ,其他无明显变化 ;而对 5 14nm激发光源 :一是有许多条谱线强度减小 ,二是许多条谱线向低波数移动了 4～ 10cm-1波数左右。这些实验结果 ,可以为研究单个红细胞的结构、功能及进一步研究病变细胞的变异提供有力的实验基础。     

DNA银纳米线的制备及其拉曼光谱

根据DNA分子的静电自组装性质,利用加热和紫外照射相结合的方法制备出大小均匀,粒径约为7.8 nm的呈正电性的银纳米颗粒。在预先梳直的小牛胸腺DNA模板上合成了长约2 μm、直径约30 nm、银颗粒较均匀分布的银纳米线。拉曼光谱表明：银颗粒主要结合在DNA主链上,同时脱氧核糖和碱基的振动峰也受到影响。磷酸根骨架的伸缩振动峰782和1 098 cm-1的强度明显减少,且谱线782移动到791 cm-1。脱氧核糖C—O的伸缩特征峰1 011和1 050 cm-1分别移动到1 030和1 064 cm-1。碱基的特征峰1 372,1 334, 1 304和728 cm-1分别移动到1 368,1 320,1 294和731 cm-1。     

Bi4Ge3O12晶体及其熔体结构的高温拉曼光谱研究

研究了BGO晶体在不同温度下(在300-1323 K的温度范围)的拉曼光谱及其熔体的高温拉曼光谱,分析了BGO晶体结构随温度变化的规律及BGO熔体的结构特征.随着温度的升高,BGO晶体的拉曼光谱谱峰都不同程度地向低波数方向移动,也存在不同程度的展宽,同时强度减弱.另外,在BGO熔体中存在[GeO4]和[BiO6]的结构基团;但两种结构之间的联键消失,即在熔体中二者是相互独立的生长基元.     

Vibrational Spectroscopy of Xanthoxyline Crystals and DFT Calculations

The Fourier transform infrared and Fourier transform Raman spectra of xanthoxyline crystals are reported, along with ab initio computations of the vibrational spectrum of the xanthoxyline molecule. The infrared and Raman spectra were recorded at 300?K in the 400- to 4,000- and 40- to 4,000-cm^?1 intervals, respectively. The vibrational wave numbers and wave vectors were obtained from a density functional computation with the 6-31 G(d,p) basis set and the B3LYP approximation to the exchange correlation functional. Comparison with the theoretical results allows assignment of normal modes to the prominent features of the recorded spectra.     

茶氨酸拉曼光谱分析

采用显微共焦拉曼光谱技术测试研究了L-茶氨酸,得到了L-茶氨酸的拉曼谱图,发现在250～1 700和2 800～3 000cm-1能够观测到明显的拉曼信号;通过对谱峰进行归属和分析,得到了不同波数范围内的特征振动模式;其中,在321,900,938,1 153,1 312,1 358,1 454和1 647cm-1找到8个较强的拉曼信号,可作为L-茶氨酸的特征峰。结果表明:拉曼光谱可能成为一种直接、准确和快速的检测茶氨酸的方法。     

AMP和DNA的银溶胶增强拉曼光谱

本文报道了生物分子5‘-腺苷磷酸（AMP）和脱氧核糖核酸（DNA）在银溶胶中的增强拉曼光谱。实验结果表明用银溶胶增加方法可以得到在较低浓度下、几乎不受光干扰的增强拉曼光谱。与固体AMP和DNA拉曼光谱进行比较,发现谱峰有很好的一致性,但也存在差异,如对应于固体AMP中715cm^-1处的腺嘌呤的呼吸振动峰加强,并位移到723cm^-1处,813cm^-1处的磷酸酯的对称伸缩振动峰消失了;在DNA中核糖环的振动峰明显加强,A,T,C,G四种碱基的峰也得到了不同程度的增强。通过对实验结果的分析,推测了AMP和DNA在银溶胶界面的吸附状态和分子结构。     

Crystal → nematic phase transition in the liquid crystalline system 1‐isothiocyanato‐4‐(trans‐4‐propylcyclohexyl) benzene (3CHBT) probed by temperature‐dependent micro‐Raman study and DFT calculations

Raman spectra of 3CHBT in unoriented form were recorded at 14 different temperature measurements in the range 25–55 °C, which covers the crystal → nematic (N) phase transition, and the Raman signatures of the phase transition were identified. The wavenumber shifts and linewidth changes of Raman marker bands with varying temperature were determined. The assignments of important vibrational modes of 3CHBT were also made using the experimentally observed Raman and infrared spectra, calculated wavenumbers, and potential energy distribution. The DFT calculations using the B3LYP method employing 6‐31G functional were performed for geometry optimization and vibrational spectra of monomer and dimer of 3CHBT. The analysis of the vibrational bands, especially the variation of their peak position as a function of temperature in two different spectral regions, 1150–1275 cm⁻¹ and 1950–2300 cm⁻¹, is discussed in detail. Both the linewidth and peak position of the ( C H ) in‐plane bending and ν(NCS) modes, which give Raman signatures of the crystal → N phase transition, are discussed in detail. The molecular dynamics of this transition has also been discussed. We propose the co‐existence of two types of dimers, one in parallel and the other in antiparallel arrangement, while going to the nematic phase. The structure of the nematic phase in bulk has also been proposed in terms of these dimers. The red shift of the ν(NCS) band and blue shift of almost all other ring modes show increased intermolecular interaction between the aromatic rings and decreased intermolecular interaction between two  NCS groups in the nematic phase. Copyright © 2009 John Wiley & Sons, Ltd.     

Raman Spectrum Study on the Doping Effect in LiNbO3: MgO Crystals

Raman spectra of LiNbO₃: MgO crystals have been obtained and compared with Raman spectra of pure LiNbO₃ crystals. For both of the two kinds of Raman active modes (4A₁+9E), no changes of the numbers, frequency-shifts, and relative intensities of the Raman spectral lines are found. However, it is observed that some modes coupled to each other at room temperature. The observed modes coupling phenomena, disappeared at low temperature. It is shown from these results that the Raman spectral lines of A₁ (TO) and E (TO) vibrational modes are mainly determined by the (NbO₆) oxygen octahedra characteristic groups of LiNbO₃ crystals.     

荧光材料Y_2O_3:Eu变温拉曼光谱分析

本文用显微拉曼谱仪在波长为785 nm的激光激发下,对Y2O3:Eu陶瓷在温度83-473 K间进行了系统的变温拉曼实验研究。实验发现Y2O3:Eu的一些振动模在低温下没有出现,只有当温度达到一定值之后才可以被观察到,分析表明这是由于温度变化引起的简并振动模式分裂。此外,Y2O3:Eu的拉曼峰位、半高全峰宽(FWHM)也是温度的非线性函数,且不同的拉曼峰遵循不同的函数关系,本文分析这是由于晶格的各向异性导致的。     

Changes in spectral features with varying mole fractions of anisaldehyde in binary mixtures

Raman and IR spectra of neat anisaldehyde (4‐methoxybenzaldehyde (4MeOBz)) and its binary mixtures (in polar and nonpolar solvents) with varying mole fraction of 4MeOBz were investigated. The concentration dependence of the wavenumber position and line width (full width at half maximum, FWHM) was analyzed to study the interaction of the solute vibrational modes with the microscopic solvent environment. The wavenumbers of Raman modes of 4MeOBz, namely, the carbonyl stretching, aldehydic δ (C H) and ring‐breathing modes, showed a linear variation in the peak position for varying concentrations of 4MeOBz in the different solvents. The dependence of Raman line width with concentration of 4MeOBz of these modes was also taken into account. The solute–solvent interaction is stronger in 2‐propanol and acetonitrile because of the formation of hydrogen bonds between them, whereas in benzene the interaction is too weak to affect the Raman modes. The modes, ν (CO) in 2‐propanol and aldehydic δ (C H) in acetonitrile, gave a Gaussian‐type line width variation, which was explained by the concentration fluctuation model, and the linear variation of the line widths was also interpreted by solute–solvent interactions. IR spectra were taken for these binary mixtures, which also give further support to these data. Copyright © 2006 John Wiley & Sons, Ltd.     

三硼酸铯和硼酸铯锂晶体的晶格振动光谱研究

本文对新型非线性光学晶体三硼酸铯（ＣｓＢ３Ｏ５∶ＣＢＯ）和硼酸铯锂（ＣｓＬｉＢ６Ｏ１０∶ＣＬＢＯ）进行了晶格振动光谱研究。首先对两种晶体的基本晶格振动模进行了对称性分类,记录了两种晶体低温下的拉曼光谱和室温下的红外反射光谱,对晶体的晶格振动模进行了认定,将振动模归属于平面六元环（Ｂ３Ｏ６）和四面体（ＢＯ４）。然后比较了ＣＢＯ,ＣＬＢＯ和ＬＢＯ（ＬｉＢ３Ｏ５）三种晶体的晶格振动光谱,讨论了阳离子对振动光谱的影响。另外,还讨论了硼酸盐晶体晶格振动模ＬＯ ＴＯ分裂的大小与晶体非线性光学系数之间的关系。     

Hydrogen local vibrational modes in zinc oxide

Using Raman backscattering spectroscopy we have observed six local vibrational modes in as-grown state-of-the-art nominally undoped zinc oxide single crystals. The local vibrational modes are located at nu=2854, 2890, 2918, 2948, 2988, and 3096 cm(-1). Some specimens were annealed up to 950 degrees C to remove hydrogen. A subsequent Raman backscattering measurement revealed that the local vibrational modes disappeared. This establishes that the observed local vibrational modes are caused by the presence of hydrogen in the ZnO crystals.