二维拉曼相关光谱研究稀土离子Eu3+对血红蛋白结构的影响

用二维拉曼相关光谱技术研究了稀土离子Eu³⁺对血红蛋白结构的影响.结果表明,以Eu³⁺浓度作为微扰,血红蛋白的结构敏感谱带均对微扰敏感,氧化态和自旋态标志谱带1374和1640cm^-1发生了同步变化,且明显先于其它谱带强度的变化,稀土离子Eu³⁺对血红蛋白的作用主要是影响它的氧化态和自旋态.     

菠萝蛋白酶催化合成寡聚L-酪氨酸

以菠萝蛋白酶为催化剂从L-酪氨酸甲酯聚合得到寡聚L-酪氨酸(O-L-Try)。 以0.8 U/mL蛋白酶在体积分数为7.5%的二甲亚砜(DMSO)缓冲液(pH=7.5,0.2 mol/L)中催化0.23 g/mL L-酪氨酸甲酯在50 ℃下聚合反应5 h后,O-L-Try产率达到65%。 通过基质辅助激光解吸电离飞行时间质谱(MALDI-TOF-MS)、氢核磁共振波谱仪(¹H NMR)、拉曼光谱、傅里叶变换红外光谱仪(FTIR)等技术手段表征了O-L-Try结构和性能特征。 结果表明,MALDI-TOF-MS测定的O-L-Try的聚合度主要为10。 ¹H NMR谱图分析得到的O-L-Try的平均聚合度为8。 拉曼光谱显示,O-L-Try的肽键特征峰位于1623 cm^-1(酰胺Ⅰ带)、1447 cm^-1(酰胺Ⅱ带)、1270 cm^-1(酰胺Ⅲ带)和648 cm^-1(酰胺Ⅳ带)。     

稀土乙酰丙酮络合物的拉曼光谱(Ⅱ)

本文从拉曼光谱观察水合分子对无水、一水、三水稀土乙酰丙酮络合物的金属-氧(M-O)拉伸振动带的影响,发现无水络合物在400cm^-1附近只有一个振动带,一水络合物在400和415cm^-1附近有两个强度不等的振动带,它们的M-O振动频率随原子序数变化都呈“四分组”效应,而三水络合物400cm^-1附近带变形,且随轻、重稀土而异,从而干扰了镧系变化规律,没有系统的“四分组”效应。由于一水络合物415cm^-1附近带随脱水而消失,吸水而复现的可逆实验事实,修正了前文对415cm^-1附近带的指定,而归属于(M-O)H₂。络合物M-O拉伸带随水合分子变化反映灵敏,出现特征带形。     

红外光谱酰胺Ⅲ带用于蛋白质二级结构的测定研究

用甲醇对BSA和RaseA等蛋白质进行变性处理,结合蛋白质酰胺带的拟合结果对酰胺带各二级结构的谱峰进行了初步指认:1330～1290cm^-1为α-螺旋;1295～1265cm^-1为β-转角;1270～1245cm^-1为无规卷曲;1250～1220cm^-1为β-折叠.依据这些谱峰归属,对一些已知二级结构的蛋白质进行了测定,所得结果与X射线衍射数据以及酰胺带的定量结果基本一致.     

四(对-十八酰氧基)苯基卟啉及其过渡金属配合物的合成及红外光声光谱研究

合成了5,10,15,20-四(对-十八酰氧基)苯基卟啉及其Mn(Ⅲ),Fe(Ⅲ),Co(Ⅱ),Ni(Ⅱ),Cu(Ⅱ)和Zn(Ⅱ)配合物,用元素分析和紫外-可见光谱等方法进行了表征.研究了这7种卟啉化合物在3600～190cm^-1范围内的傅里叶变换红外光声光谱,对主要谱带进行了经验归属.结果表明,3318.0及968.4cm^-1处的吸收谱带分别是四(对-十八酰氧基)苯基卟啉N-H键的伸缩振动和面内弯曲振动,生成配合物后这些谱带消失.243cm^-1附近的吸收谱带是M-N键伸缩振动和卟啉环变形振动的复合振动,321cm^-1附近的吸收谱带是M-Cl键的伸缩振动,金属敏感带出现在1350,1018,995,802,740,632和232cm^-1附近.     

四(对-辛酰氧基)苯基卟啉配合物的红外光声光谱

测试并研究了四(对-辛酰氧基)苯基卟啉及其Mn(Ⅲ)、Fe(Ⅲ)、co(Ⅱ)、Ni(Ⅱ)、Cu(Ⅱ)、Zn(Ⅱ)配合物在3600～190cm^-1范围内的傅立叶变换红外光声光谱,对主要谱带进行了经验归属.结果表明:3318.0和968.0cm^-1处的吸收谱带分别是四(对-辛酰氧基)苯基卟啉N-H键的伸缩振动和面内弯曲振动,生成配合物后这些谱带消失.～243cm^-1处的吸收谱带是M-N键伸缩振动和卟啉环变形振动的复合振动,～320cm^-1处的吸收谱带是M-Cl键的伸缩振动,金属敏感带出现在1504,1350,1022,995,796和235cm^-1处.     

超高分子量聚乙烯的红外光谱的特性研究

研究了超高分子量聚乙烯(M_w>1×10⁵)的红外光谱-温度特性.3条非晶谱带(1368、1352和1304cm^-1)的吸收强度均随温度升高而增大,但都比普通分子量聚乙烯增加的小,尤以高于140℃更甚.分子链中次甲基的近程构象序列分布随温度的变化不受分子量的影响,但旁式构象序列分布则随温度升高而增大.升温和降温过程的红外光谱均表明1352和1304cm^-1两谱带随结晶状态的变化比1368cm^-1更敏感.     

稀土乙酰丙酮络合物的激光拉曼和红外光谱(Ⅰ)

本文测定了15个一水稀土乙酰丙酮络合物的激光拉曼和红外光谱,在401、415cm~(-1)附近的拉曼谱带对不同稀土离子表现敏感,它们随原子序数变化呈现“四分组”效应,这是第一次在振动光谱中观察到的镧系递变规律。该系列络合物的振动频率变化亦符合镧系“斜W”效应的规律,这些特征规律为确认401、415cm^-1附近谱带为M-O拉伸振动提供了最好的证据。实验结果同时可用于讨论M-O键的性质。     

新鲜宫颈癌组织的拉曼光谱研究

采用便携式拉曼光谱仪对新鲜宫颈癌组织、 宫颈上皮内瘤变Ⅲ级(CIN Ⅲ)组织及正常宫颈组织进行检测, 通过光谱特征峰分析比较了各组织中化学成分的差异, 归纳了3类组织的拉曼光谱特征及区别. 正常组织以脂类特征峰(817, 1127, 1176, 1450, 1769 cm^-1)为主, 而宫颈癌和宫颈上皮内瘤变Ⅲ级组织则以蛋白特征峰(755, 1003, 1372, 1542, 1577 cm^-1)为主. 病变组织的主要区别在于宫颈上皮内瘤变Ⅲ级组织在853和1542 cm^-1处出现了较明显的蛋白特征峰; 宫颈癌组织则含有明显的核酸特征峰(784, 1094, 1345 cm^-1). 通过特征峰归属及分析发现, 3类组织在磷酸二酯基团形成氢键的能力、 DNA的相对含量、 亚甲基的无序性、 酰胺Ⅰ带的CO变形振动及类胡萝卜素的有无等方面存在显著差异. 表明拉曼光谱可检测宫颈癌组织, 探索宫颈癌与宫颈上皮内瘤变Ⅲ级的联系与区别, 以早期诊断宫颈癌, 具有良好的临床应用潜力.     

NaNO3和NaClO4在N,N-二甲基甲酰胺中的离子溶剂化

利用红外光谱研究了NaNO₃和NaClO₄在N,N-二甲基甲酰胺(DMF)溶剂中发生离子-溶剂和离子-离子的相互作用, 分析结果表明, DMF的OC-N谱带发生了明显的变化. 定量计算了在Na⁺浓度为0.22~1.24 mol/kg范围内的溶剂化数为1~4. 对谱图中酰胺基上C-N和CO的特征峰强度随Na⁺浓度变化的对比, 推测离子溶剂化作用导致DMF的酰胺基内部形成共轭键. 利用量子化学方法进行优化及热力学性质计算, 得到C-N键伸缩振动频率及红外光谱强度变化规律. 优化结构与实验结论相符合. 由NaNO₃的ν₂谱带及NaClO₄的ν₁谱带的解析得到溶液中阴离子缔合效应的一般规律, 并通过阴离子缔合特征峰与酰胺基上的N-C-N面外振动峰(865 cm^-1)的变化情况, 讨论了溶液中的离子溶剂化作用.     

Surface enhanced Raman spectra of nucleic acid components adsorbed at a silver electrode

High-resolution vibrational spectra of nucleic acid components adsorbed on a silver electrode were obtained using a spectroelectrochemical method based on the large-intensity enhancement for Raman scattering at electrode surfaces.The laser surface Raman spectra of purine, adenine, adenosine, deoxyadenosine, adenine mononucleotides, adenylyl-3′, 5′-adenosine and polyriboadenylic acid were recorded in the range of 150–3500 cm^?1. The intensities of the vibrational bands were highly dependent upon the electrochemical preparation of the electrode, the applied potential and the nature of the adsorbate species. High-intensity spectra in rather dilute bulk solutions were obtained.The phosphate derivatives of adenosine exhibited strongly enhanced Raman scattering. Spectral band frequencies corresponded closely with normal Raman spectra of these molecules in solution. The adenine ring breathing mode at 740 cm^?1 and the adenine ring skeletal vibration at 1335 cm^?1 produced prominent Raman scattering. A strong band at about 240 cm^?1 for the adenine mononucleotides was attributed to silver/adsorbed phosphate group vibrations.     

Infrared spectra of cyclic ethers and their derivatives

Data for the characteristic bands of cyclic ethers are reviewed. The infrared spectra of a number of 2-mono- and 2, 5-di-substituted derivatives of tetrahydrofuran are investigated. Absorption bands at about 900 cm⁻¹ are related to pulsation vibrations, and those at about 1200 cm⁻¹ to antisymmetric skeletal vibrations, of the tetrahydrofuran ring. It is shown that to confirm the presence of a tetrahydrofuran ring in a molecule, it is necessary to take into account not only the band of valence antisymmetric vibrations of the group C-O-C (ν _C-O-C ^as 1075 cm⁻¹), but also bands due to ring pulsation vibrations (ring symmetric valence vibrations ν _sk ^s ∼ 900 cm¹).     

Vibrational spectroscopy of the sorosilicate mineral hemimorphite Zn4(OH)2Si2O7 · H2O

Raman spectroscopy complimented by infrared spectroscopy has been used to study the mineral hemimorphite from different origins. The Raman spectra show consistently similar spectra with only one sample showing additional bands due to the presence of smithsonite. Raman bands observed at 3510–3565 and 3436–3455 cm⁻¹ are assigned to OH stretching vibrations. Using a Libowitzky type formula, these OH bands provide hydrogen bond distances of 0.2910, 0.2825, 0.2762 and 0.2716 pm. Water bending modes are observed in the Raman spectrum at 1633 cm⁻¹. An intense Raman band at 930 cm⁻¹ is attributed to SiO symmetric stretching vibration of the Si₂O₇ units. Raman bands observed at 451 and 400 cm⁻¹are attributed to out-of-plane bending vibrations of the Si₂O₇ units. Raman bands at 330, 280, 168 and 132 cm⁻¹ are assigned to ZnO and OZnO vibrations.     

Infrared spectra of cyclic ethers and their derivatives

The IR spectra of six monosubstituted and of four 2,6-disubstituted 1,4-dioxanes have been studied in the 650–1800cm^–1 region. The assignment of the bands due to the vibrations of the 1,4-dioxane ring and to the deformation vibrations of the methylene groups of the ring is given. The appearance of a whole series of new absorption bands on passing from unsubstituted 1,4-dioxane to its derivatives is explained by the change in the symmetry of the molecule and the removal of the prohibition from the vibrations previously inactive in the IR spectra connected with this reduction in symmetry. It is proposed to use, in order to confirm the presence of a 1,4-dioxane ring in a molecule from the results of IR spectroscopy, not only the 1126-cm^–1 band but the whole group of bands lying in the frequency ranges 800–950, 1000–1150, and 1200–1300 cm^–1.For part I, see [3].     

Vibrational spectra and infrared dichroism of tetraphenyl-silane,Ph4Si. II.

Vibrational spectra of Ph₄Si have been studied from 600 to 20 cm^?1 in solution, in the melt and in the crystalline state. The assignments proposed for the substituent sensitive benzene ring vibrations, for the skeletal bending modes and ring librations have been supported by polarized IR and Raman measurements. The crystal spectra are interpreted on the basis of the S₄ site symmetry of the molecules in the crystal. Two skeletal bending and four ring librational modes are supposed to appear below 120 cm^?1, in the range of the lattice vibrations.     

Raman spectroscopic investigation of the antimalarial agent mefloquine

The antimalarial agent mefloquine was investigated using Fourier transform near-infrared (FT NIR) Raman and FT IR spectroscopy. The IR and Raman spectra were calculated with the help of density functional theory (DFT) and a very good agreement with the experimental spectra was achieved. These DFT calculations were applied to unambiguously assign the prominent features in the experimental vibrational spectra. The calculation of the potential energy distribution (PED) and the atomic displacements provide further valuable insight into the molecular vibrations. The most prominent NIR Raman bands at 1,363 cm⁻¹ and 1,434 cm⁻¹ are due to C=C stretching (in the quinoline part of mefloquine) and CH₂ wagging vibrations, while the most intense IR peaks at 1,314 cm⁻¹; 1,147 cm⁻¹; and 1,109 cm⁻¹ mainly consist of ring breathings and δCH (quinoline); C–F stretchings; and asymmetric ring breathings, C–O stretching as well as CH₂ twisting/rockings located at the piperidine moiety. Since the active agent (mefloquine) is usually present in very low concentrations within the biological samples, UV resonance Raman spectra of physiological solutions of mefloquine were recorded. By employing the detailed non-resonant mode assignment it was also possible to unambiguously identify the resonantly enhanced modes at 1,619 cm⁻¹, 1,603 cm⁻¹ and 1,586 cm⁻¹ in the UV Raman spectra as high symmetric C=C stretching vibrations in the quinoline part of mefloquine. These spectroscopic results are important for the interpretation of upcoming in vitro and in vivo mefloquine target interaction experiments.     

Different level of fluorescence in Raman spectra of montmorillonites

The paper presents the study of selected montmorillonite standards by Raman spectroscopy and microscopy supported by elemental analysis, X-ray powder diffraction analysis and thermal analysis. Dispersive Raman spectroscopy with excitation lasers of 532 nm and 780 nm, dispersive Raman microscopy with excitation laser of 532 nm and 100× magnifying lens, and Fourier Transform-Raman spectroscopy with excitation laser of 1064 nm were used for the analysis of four montmorillonites (Kunipia-F, SWy-2, STx-1b and SAz-2). These mineral standards differed mainly in the type of interlayer cation and substitution of octahedral aluminium by magnesium or iron. A comparison of measured Raman spectra of montmorillonite with regard to their level of fluorescence and the presence of characteristic spectral bands was carried out. Almost all measured spectra of montmorillonites were significantly affected by fluorescence and only one sample was influenced by fluorescence slightly or not at all. In the spectra of tested montmorillonites, several characteristic Raman bands were found. The most intensive band at 96 cm⁻¹ belongs to deformation vibrations of interlayer cations. The band at 200 cm⁻¹ corresponds to deformation vibrations of the AlO₆ octahedron and at 710 cm⁻¹ can be assigned to deformation vibrations of the SiO₄ tetrahedron. The band at 3620 cm⁻¹ corresponds to the stretching vibration of structural OH groups in montmorillonites.     

Thermal decomposition of the hydrotalcite

Summary A combination of thermogravimetry and hot stage Raman spectroscopy has been used to study the thermal decomposition of the synthesised zinc substituted takovite Zn₆Al₂CO₃(OH)₁₆·4H₂O. Thermogravimetry reveals seven mass loss steps at 52, 135, 174, 237, 265, 590 and ~780°C. MS shows that the first two mass loss steps are due to dehydration, the next two to dehydroxylation and the mass loss step at 265°C to combined dehydroxylation and decarbonation. The two higher mass loss steps are attributed to decarbonation. Raman spectra of the hydroxyl stretching region over the 25 to 200°C temperature range, enable identification of bands attributed to water stretching vibrations, MOH stretching modes and strongly hydrogen bonded CO₃^2--water bands. CO₃^2- symmetric stretching modes are observed at 1077 and 1060 cm^-1. One possible model is that the band at 1077 cm^-1is ascribed to the CO₃^2- units bonded to one OH unit and the band at 1092 cm^-1is due to the CO₃^2- units bonded to two OH units from the Zn-takovite surface. Thermogravimetric analysis when combined with hot stage Raman spectroscopy forms a very powerful technique for the study of the thermal decomposition of minerals such as hydrotalcites.</o:p>     

Neutron inelastic scattering spectra of strongly hydrogen bonded acid oxalates NaHC2O4, KHC2O4 and LiHC2O4

Neutron inelastic scattering spectra of NaHC₂O₄, KHC₂O₄ crystals at 80 K have been recorded in the 2200-200 cm^?1 range. The lithium acid salt was also studied at different temperatures. NIS spectra are compared to the corresponding infrared and Raman spectra and an assignment is proposed. Two strong bands near 1500 and 1100 cm^?1 are assigned to δ(OH) and γ(OH) vibrations, respectively, while five weak bands below 900 cm^?1 are associated with skeletal modes, mainly bending vibrations. The OH stretching vibration is not observed and is believed to be hidden by other bands; the peak intensity must be low because of its band width which is of the order of a few hundreds wavenumbers.     

Excitation conversion in excimers and exciplexes of aromatic hydrocarbons

Flurorescence spectra of a number of aromatic hydrocarbons, their excimers and exciplexes with diethylaniline have been measured in n-hexane under aerobic conditions. It has been found that the value of the red shift of the structureless excimer or exciplex band in reference to the monomer fluorescence band is about 4200 or 3000 cm⁻¹, respectively. For indole—ethanol exciplexes the red shift was about 3700 cm⁻¹. It is suggested, that the shift depends on the intramolecular vibrations in the quencher accepting the vibrational energy from the electronically excited donor molecule. It has been proposed that excimer and exciplex fluorescence occurs due to the donor emission of a number of quanta from the virtual levels.