四苯基卟啉及其衍生物的结构与性质研究(Ⅳ)——二质子四苯基卟啉及其衍生物的光谱、pKa与取代基常数间的线性关系

以HMO法剖析了二质子四苯基卟啉(H₂TPP²⁺)及其衍生物的紫外-可见光谱,确定了四苯基卟啉(TPP)和H₂TPP²⁺及其衍生物的λ_max、pK_a与取代基常数σ间的线性关系。     

萘酰亚胺类荧光染料及共聚型荧光聚氨酯乳液的合成与性能

首先以4-溴-1,8-萘酐、2-氨基-1,3-丙二醇和甲醇钠为原料, 经亚胺化和取代两步反应合成出4-甲氧基-N-(2-羟基-1-羟甲基乙基)-1, 8-萘酰亚胺(MHHNA)活性荧光染料, 然后将其作为扩链剂通过相反转自乳化法制备出了共聚型荧光聚氨酯(PU) (PU-MHHNA)乳液, 并分别采用核磁共振氢谱(¹H NMR)、核磁共振碳谱(¹³CNMR)、元素分析、傅里叶变换红外(FTIR)光谱、紫外-可见(UV-Vis)吸收光谱、荧光光谱、粒度分析、氙灯老化等方法对所得荧光染料的化学结构、PU乳液及乳胶膜的性能进行了表征. 结果表明, MHHNA和PU-MHHNA的荧光量子产率分别为0.73 和0.92, MHHNA的用量对所得PU乳液的胶体性质没有明显影响. PU-MHHNA的丙酮溶液在UV-Vis 吸收光谱上的最大吸收波长(λ_max)为360.6 nm, 在荧光光谱上的最大激发波长(λ_ex)和最大发射波长(λ_em)分别为362和435 nm. 随着温度的升高, PU-MHHNA的荧光强度逐渐降低. PU-MHHNA乳胶膜的耐光色牢度和耐溶剂色牢度均明显高于共混型荧光聚氨酯(PU/MBNA)乳胶膜.     

二茂铁亚胺及其环汞化合物的薄层色谱及紫外-可见、红外光谱特征

通过测定R^f值对比研究了二茂铁亚胺及其环汞化合物的色谱亲和性,发现环汞化合物比未汞化的二茂铁亚胺具有较高的R_f值,并用N→Hg分子内配位作用给予解释。分析取代基效应表明,亚胺氮上电子密度越高,R_f值越小。紫外可见光谱表明,环汞化合物分子中存在有N→Hg分子内配位作用。研究了N-Ar环和亚胺碳上的取代基效应对紫外光谱的影响,与N-Ar环上无取代基时相比,π→π^*CT跃迁带的最大吸收波长移动值△λ_max和Hammett-Brown常数σ⁺之间存在良好的线性关系。考察了二茂铁红外光谱规则对所研究体系的适用情况。     

2-(4-咔唑-1-基-苯基)-1H-苯并咪唑的合成及其光学性质

以邻苯二胺与4-(咔唑-1-基)苯甲醛为原料,合成了一种新型苯并咪唑衍生物--2-(4-咔唑-1-基-苯基)-1H-苯并咪唑(2),其结构经¹H NMR, ¹³C NMR, MS（ESI), IR和元素分析表征。通过理论计算,结合UV-Vis和单光子荧光光谱研究了其光学性质,结果表明：2在二氯甲烷,乙酸乙酯,乙醇,乙腈和DMF中的λ_max均位于292 nm和330 nm 附近, λ_em分别为389 nm, 379 nm, 395 nm, 400 nm和390 nm。     

一种共轭结构三苯胺衍生物的制备及光学性质

通过固相Wittig反应合成了一种π共轭结构有机荧光化合物。其结构经¹HNMR、¹³CNMR、IR及ESI-MS表征。通过实验研究了化合物的UV-Vis和荧光光谱并采用理论计算进行了光谱机理解释。目标化合物在二氯甲烷、乙酸乙酯、乙醇、乙腈和N, N-二甲基甲酰胺中的最大吸收波长λ_max均位于310 和380 nm处,在上述溶剂中的最强荧光发射波长λ_em分别为438、436、439、448和451 nm。      

上转换荧光化合物DMSSB与CSSB的合成、结构与光物理性质

以苯并噻唑为电子受体,以双苯乙烯基为共轭桥链,分别以二甲基胺和咔唑为电子给体合成了2个新的有机化合物DMSSB(反式,反式-2-{4-[(4-N,N-二甲基胺)苯乙烯基]苯乙烯基}-1,3-苯并噻唑)和CSSB(反式,反式-2-{4-[(4-N-咔唑)苯乙烯基]苯乙烯基}-1,3-苯并噻唑).用X射线衍射方法测定了CSSB的晶体结构.用波长为800nm的激光激发时,DMSSB与CSSB在THF中分别发出强的上转换橙色(λ_max=589nm)和蓝绿色荧光(λ_max=488nm).2个化合物在不同溶剂中的光物理数据和理论计算结果表明,苯并噻唑基是一个很好的电子受体.     

可溶性镍酞菁的光谱特性研究

利用UV-Vis吸收光谱、荧光光谱及半经验ZINDO/S方法,研究了4种可溶性镍酞菁(FPcNi、MePcNi、iBPcNi、iPPcNi)的电子吸收光谱和荧光光谱.研究结果表明:随着取代基的供电子能力增加,酞菁的最大吸收波长(λ_max)和发射波长(λ_em)发生红移,摩尔消光系数变小;随着溶液浓度增大,酞菁聚集体浓度增大,λ_max发生蓝移,但浓度对λ_em影响较小,同时荧光相对强度随浓度增大,出现最大值;随着溶剂配合能力的增加,λ_max、λ_em都发生红移.     

间苯二胺的电化学及紫外-可见薄层光谱电化学研究

研究了间苯二胺(MPD)在金电极和SnO₂;F膜电极上的循环伏安行为及在SnO₂;F膜电极上的紫外-可见薄层光谱电化学性质.获得了间苯二胺在SnO₂;F膜电极上电氧化的薄层恒电势电解-吸收光谱图,采用双对数法对紫外-可见薄层光谱电化学数据进行了处理.研究了间苯二胺的光谱及电化学性质,求得了间苯二胺的动力学修饰式量电位E⁰和αn等热力学参数.     

食品中苏丹红Ⅰ和辣椒红的表面增强拉曼散射(SERS)光谱与激发-发射矩阵荧光光谱鉴别

利用表面增强拉曼散射(SERS)光谱及激发-发射矩阵(EEM)荧光光谱对食品中非法添加剂苏丹红Ⅰ和合法食品添加剂辣椒红进行了定性分析和检测. SERS光谱结果表明, 苏丹红Ⅰ在低波数区域分子的扭转振动信号增强比较明显; 而辣椒红在1521和1158 cm^-1处拉曼信号增强效果比较明显; EEM荧光光谱结果表明, 苏丹红Ⅰ的乙醇溶液在P₁(λ_ex=285 nm, λ_em=345 nm)和P₂(λ_ex= 335 nm, λ_em=548 nm)处有2个明显的荧光特征峰; 而辣椒红的乙醇溶液有3个特征荧光峰, 分别为P₁(λ_ex=545 nm, λ_em=580 nm), P₂(λ_ex=560 nm, λ_em=665 nm)和P₃(λ_ex=608 nm, λ_em=672 nm).     

纳米Au-TiO2复合薄膜的溶胶-凝胶法制备、表征和性能

用溶胶-凝胶法制备了纳米Au-TiO₂复合薄膜.X射线衍射、X射线光电子能谱、原子力显微镜、紫外-可见光谱及摩擦磨损实验研究表明,复合薄膜均匀致密,Au以纳米晶粒形式均匀、不连续分散镶嵌于TiO₂基体中,纳米Au粒径为14～25nm;复合薄膜在可见光区有较强的吸收,吸收峰位置和强度与烧结温度和金的添加量有关;复合薄膜具有良好的抗磨减摩性能,在1N负荷下,摩尔分数为5%的Au-TiO₂薄膜的摩擦系数仅为0.09～0.10,耐磨寿命多于2000滑动周次.     

有机银溶胶的吸收光谱和表面增强Raman光谱研究

研究了2-氨基苯并咪唑(BIMNH₂)、LiCl、NaOEt对Ag/EtOH溶胶吸收光谱和表面增强Raman散射(SERS)光谱的影响。结果表明,少量的吸附分子BIMNH₂、LiCl、NaOEt均能改变溶胶聚集状态,从而影响其吸收光谱和SERS效应。此外,Cl^-还可与Ag、BIMNH₂形成表面络合物而增强SERS效应。对Ag溶胶体系SERS光谱的溶剂效应也作了初步研究。     

3-吡咯烷基苯并蒽酮的电子结构和光谱性质

苯并蒽酮衍生物在新型荧光材料、非线性光学材料和液晶显示材料等领域有较大的应用前景.本文采用量子化学方法优化了3-吡咯烷基苯并蒽酮的基态几何结构和第一单重激发态的几何结构,并与X射线晶体衍射实验值进行了对比.利用含时密度泛函理论(TD-DFT)的不同泛函,计算了3-吡咯烷基苯并蒽酮在气相和溶剂中的吸收和发射光谱,考察了它的电子结构和光谱特征,并分析了不同泛函、基组以及溶剂效应对吸收和发射光谱的影响.计算结果表明:3-吡咯烷基苯并蒽酮的最强吸收和发射光谱都是具有π→π*跃迁特征的电荷转移(CT)态;泛函B3LYP能较好地重现实验吸收能;而对于具有分子内电荷转移特征的激发态,泛函MPWK能较好地重现实验发射能.溶剂效应的计算表明,不同极性的溶剂对3-吡咯烷基苯并蒽酮的吸收光谱和发射光谱的影响较小.理论预测的光谱与实验结果一致.     

Yb∶YAB晶体的生长及性质

研究了ＹｂｘＹ１－ｘＡｌ３（ＢＯ３）４（Ｙｂ∶ＹＡＢ）晶体的生长及光学性质,结果表明,以Ｋ２Ｍｏ３Ｏ１０作为助熔剂生长Ｙｂ∶ＹＡＢ晶体效果较好,根据测定的Ｙｂ∶ＹＡＢ折射率计算的一类位相匹配角为θｍ（Ⅰ）＝３４°１２′,与实验测定值θｍ（Ⅰ）＝３４°３８′吻合较好。该晶体室温吸收谱在９５６和９７５ｎｍ处存在两个吸收带,适于ＩｎＧａＡｓ泵浦;室温π偏振吸收比σ偏振吸收略强;１０３和１０４μｍ处各存在一荧光峰,１０３μｍ处荧光寿命为１３７９ｍｓ;估算的发射截面数量级为１０－２１ｃｍ２     

Terahertz absorption spectra of some saccharides and their metal complexes

In this work, THz absorption spectra of some saccharides and their metal complexes were measured. The main purpose of this work is to investigate the M-O vibrations, intermolecular and intramolecular hydrogen bonds and other vibrations in the FIR region using powerful spectroscopic techniques adopting the metal-sugar complexes prepared in our laboratory. The M-O vibrations in the FIR spectra of metal-sugar complexes indicate the formation of metal complexes. The THz spectrum of glucose below 100cm(-1) was measured at first to confirm the THz experimental method. Characteristic absorption bands in the spectra of various samples are observed. THz spectra of saccharides below 100cm(-1) often have several absorption bands, and different saccharides have various absorption peaks in the THz region, which may be used to distinguish different saccharides. The differences in the number of bands observed are related to different structures of the samples, and these absorption bands are related to the collective motion of molecules. But the THz spectra of their metal complexes are different from the ligands, and no band appears in the region below 50cm(-1) at the present experimental condition, which indicates that THz spectroscopy may also be helpful to identify the formation of metal-sugar complexes, and the changes after complexation in the THz spectra below 100cm(-1) may be related to different metal ions. The metal-sugar complexes with similar crystal structures resemble mid-IR spectra, but their THz spectra may have some differences.     

Optical properties of single-walled 4 A carbon nanotubes

Optical properties of a series of finite sized hydrogenated carbon nanotubes with the smallest diameter of 4 A are studied systematically. Their absorption spectra are calculated with the localized-density-matrix method. The semiempirical MNDO parametric method 3 (PM3) Hamiltonian is employed. The finite optical gaps are predicted for the infinite long single-walled carbon nanotubes. Strong anisotropy characteristics of the dynamic polarizabilities are found for these tubes. The calculated results are in good agreement with the recent experimental findings. Further the compositions of the dipole-induced excitations are examined by projecting the corresponding density matrices onto the Hartree-Fock molecular orbital representation. Unlike the larger diameter carbon nanotubes whose absorption spectra are insensitive to the tube chiralities, the absorption spectra of 4 A single-walled carbon nanotubes depend very much on their chiralities. The chirality of the single-walled 4 A carbon nanotubes synthesized in the channels of the porous zeolites is thus determined to be (5,0) by comparing the calculated and measured absorption spectra.     

Terahertz spectroscopy of enantiopure and racemic polycrystalline valine

Experimental and computational THz (or far-infrared) spectra of polycrystalline valine samples are reported. The experimental spectra have been measured using THz time-domain spectroscopy. Spectra of the pure enantiomers, both D and L, as well as the dl racemate have been taken at room temperature and low temperature (78 K). The spectra of the pure D and L enantiomers are essentially identical, and they are markedly different from the DL racemate. In addition, a temperature-dependent study of L-valine was undertaken in which the absorption maxima were found to red shift as a function of increasing temperature. The vibrational absorption spectra (frequencies and intensities) were calculated using the harmonic approximation with the Perdew-Burke-Ernzerhof (PBE) functional, localized atomic orbital basis sets, and periodic boundary conditions. The calculated and experimental spectra are in good qualitative agreement. A general method of quantifying the degree to which a calculated mode is intermolecular versus intramolecular is demonstrated, with the intermolecular motions further separated into translational versus rotational/librational motion. This allows straightforward comparison of spectra calculated using different basis sets or other constraints.     

Specific features of UV-vis absorption spectra of cis- and trans-polythiophenes

UV-vis optical spectra of several polythiophene with number of dimers n=1, 5, 10, 15 for cis- and trans-forms were investigated. The study was done theoretically using semi-empirical AM1 (Austin Model 1) and PM3 (Parametric Method 3) methods with the appropriate molecular geometry optimization. The experimental UV-vis absorption spectra were used for verification of the both semi-empirical theoretical models. With the increasing number of dimers a red shift of the absorption edge was observed. Solvent does not play a crucial role on behavior of the absorption spectrum. A comparison of the both semi-empirical methods with the observed experimental absorption spectra is performed. Role of state dipole moments of the investigated polythiophenes in the behavior of the observed UV-vis spectra is discussed. Particular role of pi-conjugated bonds is demonstrated.     

Influence of bond lengths between substituents and mother molecule on spectral properties of pyrazoloquinolines

Absorption and luminescent spectra of several new synthesized pyrazolo-quinoline possessing different substituents are studied. Absorption spectra of all the considered compounds possess five relatively strong absorption bands at about 430, 320, 270, 253 and about 230 nm. A correlation between the bond lengths between the substituent molecule and mother molecule with the observed spectral shifts was found. Theoretical spectra obtained within semi-empirical quantum chemical AM1 calculation methods seem to be more widened compared to the experimental ones due to electron-vibration interactions. However generally a good coincidence between spectral positions between experimental and calculated spectral peak positions was achieved. The corresponding experimental spectra have an absorption edges situated at about 430 nm which appears in fairly good agreement with quantum chemical simulations, namely for absorption spectra calculated by semi-empirical AM1-method. The red shifts in the experimental luminescence spectra are a consequence of electron-vibration interactions which increase with the effective radius and polarizabilities of the particular substituents.     

Time‐dependent density functional theory studies of the electronic absorption spectra of metallophthalocyanines of group IVA

Time‐dependent density functional theory (TD‐DFT) calculations were carried out in a comparative study of the electronic absorption spectra of lead(II) phthalocyaninate (PbPc), tin(II) phthalocyaninate (SnPc), tin(IV) dichlorophalocyaninate (PcSnCl₂), germanium(II) phthalocyaninate (GePc), and germanium (IV) dichlorophalocyaninate (PcGeCl₂) with the B3LYP method and LANL2DZ basis set. Our calculated bands correspond well with the experimental results. The electronic natures of all the bands in the absorption spectra are assigned and analyzed comparatively according to the calculated electronic transition contributions. With the increase of the dielectric constant from CHCl₃ to DMSO, all the electronic absorption bands are somewhat red shift, consistent with the shift rules measured experimentally. The radius of the central metals has great influence to the absorption spectra, especially for the B bands. The influence of the radius of the central metals to the absorption spectra of PcSnCl₂ and PcGeCl₂ is smaller than to the spectra of the nonplanar MPcs (M = Pb, Sn, and Ge). Axial ligands also greatly changed the electronic absorption spectra due to the change of the orbital energy level and the molecular symmetry. © 2006 Wiley Periodicals, Inc. Int J Quantum Chem, 2007     

L-和DL-福多司坦的太赫兹光谱分析

利用太赫兹时域光谱技术(THz-TDS)在室温下对L-福多司坦和DL-福多司坦进行测量,发现L-和DL-福多司坦在THz波段都有特征吸收峰,且两者的吸收谱有明显差异.运用密度泛函理论的B3LYP方法计算了L-和DL-福多司坦在太赫兹波段的吸收谱,并对L-和DL-福多司坦的特征吸收峰进行了指认,理论计算与实验结果基本吻合.此外,还对福多司坦胶囊成品药进行了测量,发现该胶囊的吸收谱与L-福多司坦非常吻合,证明胶囊药的主要成分为L-福多司坦.这项研究对手性物质的检测以及化合物有效成分的鉴别有一定的参考作用.