π-(C_5H_5)_2TiCl_2·AlR_3系可溶性催化剂的电子自旋共振波谱

本文稿研究了Al(iC_4H_9)_3、Al(C_2H_5)_3、Al(C_2H_5)_2Cl、Al(C_2H_5)Cl_2等与π-(C_5H_5)_2TiCl_2 所形成的络合物在无溶剂以及在溶剂稀释过程中的电子自旋共振波谱。根据实验结果,作者认为未成对电子是定位在Al~(27)核一端,电子云可延伸到α氢原子位置上,并指出溶剂主要起着分散络合物的作用。     

乙酰丙酮-5,10,15,20-四取代苯基卟啉稀土铥络合物的吸收光谱

络合物Tm(g)Tppacac(g:H,O—NO_2,P—NO_2,O—Cl,m—Cl,P—Cl,P-CH_3O;HTpp:5,10,15,20-四苯基卟啉;Hacac:乙酰丙酮)在可见和红外区的吸收光谱被讨论。HTpp、H(P—CH_3O)Tpp、H(O—NO_2)Tpp、H(P—NO_2)Tpp、H(P—Cl)Tpp、H(O—Cl)Tpp和H(m-Cl)Tpp的核的N—H伸缩振动分别在3317、3318、3318、3320、3321和3324cm~(-1),取代物与HT_(pp)比较向长波位移1—7cm~(-1)。络合后,由于N—H上的氢被稀土离子取代,此带消失·络合物中的1516—1518cm~(-1)谱带在卟啉和过渡金属卟啉中不存在,它们与乙酰丙酮配位相关,是乙酰丙酮环上的C—C伸缩振动。但对Tm(O—NO_2)Tppacac和Tm(P—NO_2)Tppacac,产生强宽谱带1523和1519cm~(-1),这是由于邻、对位硝基苯基卟啉的反对称N—O伸缩振动1512和1524cm~(-1)与乙酰丙酮的C—C伸缩振动的迭加结果。TmTppacac的M—O伸缩振动在372cm~(-1),取代络合物此带向低波数发生明显位移,其位移次序为: Tm(m—Cl)Tppacac>Tm(O—Cl)Tppacac>Tm(P—Cl)Tppacac> Tm(P>NO_2)Tppacac>Tm(O—NO_2)Tppacac>Tm(P—CH_3O)Tppacac 按此次序,它们的带频率分别为350、355、356、357、360和366,向低波数位移6—27cm~(-1)。还有一些谱带,如吡咯的βC—H摇摆和C—H弯曲振动、吡咯和苯环的—C=C—伸缩振动等也参照文献进行了归属。可见谱带中,取代络合物与TmTppacac比较,大多数谱带都向长波或短波长方向发生位移。     

稀土金属卟啉的荧光光谱研究

用苯或乙醇为溶剂,在室温下测得了数种o-ClTPP和TPP稀土金属络合物的荧光发射光谱和荧光激发光谱。荧光激发光谱与相应吸收光谱相对应。除Y(Ⅲ)和Lu(Ⅲ)络合物的荧光量子产率稍大外,其它Ln(Ⅲ)络合物的荧光量子产率都在10~(-4)数量级。o-ClTPP系列络合物的荧光量子产率不小于TPP系列相应的稀土金属络合物。不同络合物的自然辐射寿命差别不显著。     

某些酸性磷膦酸酯VO(Ⅱ)络合物在氯仿中ESR研究

本文对某些酸性磷(膦)酸酯VO(Ⅱ)络合物在氯仿中室温ESR谱做了进一步的解析,并测得这类络合物在氯仿中在液氮温度下ESR波谱参数,计算了它们的键参数,对这类络合物的成键特性进行了讨论。     

一种新型芴类衍生物的光谱性质研究

合成了具有大π共轭性的对称型芴类衍生物9,9-二(2-乙基已基)-2,7-二(2-(4-甲氧基)苯-2,1-乙烯基)芴(简写为MO-Flu-MO)。通过元素分析、质谱、紫外-可见光谱和红外光谱对其进行了表征。测试了该染料在乙腈、二氯甲烷、四氢呋喃和正己烷4种不同极性溶剂中的线性吸收光谱和单光子荧光谱。结果发现溶剂效应对吸收光谱和荧光光谱表现出不同程度的影响,对产生这些光谱行为的主要原因进行了讨论。     

驱动四苯基卟啉锌(Ⅱ)-咪唑基尾式卟啉铁(Ⅲ)超分子自组装的配位键:荧光光谱和1H NMR谱的研究

以荧光光谱和1HNMR谱研究了驱动四苯基卟啉锌 (Ⅱ ) [Zn(TPP) ] 咪唑基尾式卟啉铁 (Ⅲ ) [Fe(p ImEPTPP)Cl]超分子自组装的配位键。研究表明 ,Fe(p ImEPTPP)Cl加入到Zn(TPP)二氯甲烷溶液引起的荧光猝灭是前者的尾端咪唑基配位到后者中心离子Zn2 的结果。在Zn(TPP) /Fe(p ImEPTPP)Cl体系中分别加入哌啶、咪唑和吡啶等Lewis碱后荧光光谱变化提供了配位键生成的进一步证据。Zn(TPP) /Fe(p ImEPTPP)Cl体系的1HNMR谱中的咪唑基质子化学位移的变化 ,再次证明了配位键的生成     

5α-雄甾烷-3,17二-酮在一元溶剂中的红外光谱

在20种不同纯有机溶剂中,研究了5α-雄甾烷-3,17-二酮C3位和C17位羰基的红外光谱。将其羰基伸缩振动频率分别与经验溶剂参数如溶剂接受数AN、Brownstein的溶剂参数S和Schleyer线性自由能方程参数G值进行了相关分析。结果表明,C3位C=O在一元溶剂体系中出现2种谱带,而C17位C=O则出现3种谱带。羰基伸缩振动频率位移与AN值、G值具有较好的线性相关性,而在非醇溶剂中与S值线性相关较差。采用简单化合物丙酮分别对溶剂硝基苯、乙腈、二氯甲烷和氯仿的S值进行修正,并将复杂甾酮化合物5α-雄甾烷-3,17-二酮的羰基红外频率与S修正值进行线性分析,相关性良好。     

5α-雄甾烷-3,17-二酮在一元溶剂的红外光谱

在20种不同纯有机溶剂中,研究了5a-雄甾烷-3,17-二酮C3位和C17位羰基的红外光谱.将其羰基伸缩振动频率分别与经验溶剂参数如溶剂接受数AN、Brownstein的溶剂参数S和Schleyer线性自由能方程参数G值进行了相关分析.结果表明,C3位C=O在一元溶剂体系中出现2种谱带,而C17位C=O则出现3种谱带.羰基伸缩振动频率位移与AN值、G值具有较好的线性相关性,而在非醇溶剂中与S值线性相关较差.采用简单化合物丙酮分别对溶剂硝基苯、乙腈、二氯甲烷和氯仿的S值进行修正,并将复杂甾酮化合物5a-雄甾烷-3,17-二酮的羰基红外频率与S修正值进行线性分析,相关性良好.     

Tl(Ⅲ)-Cu(Ⅱ)-EDTA-H2O2-DPC体系反应机理研究

本文用光度法研究了在弱酸性介质中 ,Tl(Ⅲ ) Cu(Ⅱ ) EDTA H2 O2 DPC体系的反应机理。实验结果表明 ,该体系的反应机理是基于Tl(Ⅲ )置换出Cu(Ⅱ ) EDTA络合物中的Cu(Ⅱ ) ,Cu(Ⅱ )催化H2 O2 氧化二苯碳酰二肼生成二苯卡巴腙 ,然后Cu(Ⅱ )与二苯卡巴腙络合 ,生成有色络合物被氯仿萃取 ,在有机相中其络合物的最大吸收波长为 550nm。     

两种新型二氯代苯基卟啉-5-氟尿嘧啶衍生物的合成与表征

用5-[4-(5-溴戊氧基)苯基]-10,15,20-三(3,4-二氯苯基)卟啉或5-[4-(6-溴己氧基)苯基]-10,15,20-三(3,4-二氯苯基)卟啉与5-氟尿嘧啶反应,合成了1-[5-(4-戊氧苯基)-10,15,20-三(3,4-二氯苯基)卟啉]-5-氟尿嘧啶(A)和1-[5-(4-己氧苯基)-10,15,20-三(3,4-二氯苯基)卟啉]-5-氟尿嘧啶(B),产率分别为29.92%和30.01%。并通过红外光谱、紫外可见光谱、核磁共振谱和质谱表征了其结构。对目标化合物的合成条件进行了研究,结果表明:以DMF为溶剂,反应温度为115℃,反应时间2h,产率较高;采用硅胶G(200—300目)装柱,以氯仿和氯仿∶乙醚(V∶V=50∶1)为洗脱液,柱层析,再用氯仿:丙酮(V∶V=7∶1)洗脱产品色带,分离效果较好。     

Photophysical parameters and laser performance of 3-(4′-dimethylaminophenyl)-1-(2-furanyl)prop-2-en-1-one (DMAFP): A new laser dye

The spectral properties such as singlet absorption, molar absorptivity, emission spectra, fluorescence quantum yield and excited state lifetime of 3-(4′-dimethylaminophenyl)-1-(2-furanyl)prop-2-en-1-one (DMAFP) have been determined in different solvents. DMAFP dye exhibits a large red shift in both electronic absorption and emission spectra as the solvent polarity increases, indicating a large change in the dipole moment of molecules upon excitation. A crystalline solid of DMAFP gives an excimer like emission at 566 nm due to the excitation of molecular aggregates. This is expected from the idealized crystal structure of the dye that belongs to the B-type class of Steven's classification. The ground and excited state protonation constants of DMAFP are calculated and amounted to 1.71 and 8.3, respectively. DMAFP acts as a good laser dye upon pumping with nitrogen laser (λ_ex=337.1 nm) in chloroform, methylene chloride and dioxane and gives laser emission in the range 460–590 nm. The laser parameters such as the tuning range, gain coefficient (α), emission cross section (σ_e) and half-life energy (E_1/2) are calculated. The photoreactivity and net photochemical quantum yield of DMAFP in chloromethane solvents are also studied.     

Solvent and temperature-dependent conductive behavior of poly(3-hexylthiophene)

Impedance characterization at different temperatures has been used to investigate the conductive behavior of Poly(3-hexylthiophene) (P3HT), prepared in different solvents, as the semiconductor layer in organic multilayer capacitor. It has been found that the P3HT films using chloroform and toluene solvents exhibit an enhancement in conductivity by heating following an Arrhenius law with an activation energy transition from 0.004 to 0.026 eV and from 0.002 to 0.015 eV at ~313 K, respectively, which originates from band tail hopping that occurs around the Fermi edge. The boiling point of the used solvents can affect P3HT crystallization process, which causes the difference in conduction and activation energy.     

Two-photon fluorescence properties of a styrylpyridinium derivative organic chromophore in different solvents

The fluorescence properties of a new two-photon absorption chromophore in dimethyl formamide, methanol, acetone, benzyl alcohol, methylene chloride and chloroform are reported. The lifetime, intensity and central wavelength of the fluorescence signal vary significantly in different solvents. The fluorescence properties are explained by using the twisted intra-molecular charge-transfer model, the viscosity of the solvents and the formation of the hydrogen bond. For the dye in all solvents, the longer the fluorescence lifetime, the higher the fluorescence intensity. Generally, the higher the dipole moments, the longer the central wavelengths of the dye. PACS 42.65.-k; 42.65.Ky; 87.64.Ni     

Rheological Behavior of Polyarylsulfone 1‐Butyl‐3‐Methylimidazolium Chloride Solutions

Polyarylsufone polymers are engineering thermoplastics that can only be dissolved in polar solvents. We found that polyarylsufone has good solubility in ionic liquid (IL) with IL being a new kind of green solvent; thus, ILs are potential substitutes for conventional molecular solvents. However, the thermodynamics in ionic liquids are different then those in conventional solvents, so ILs as solvents have attracted enormous attention recently. Rheological behavior is an important factor in polymer material processing. The rheological behavior of polyarylsulfone (PASF) in both N, N,‐dimethylacetamide (DMAc) and ionic liquid 1‐butyl‐3‐methylimidazolium chloride [(Bmim) Cl] were studied in this paper as a function of concentration for concentrated solutions. It is interesting that the rheological behavior of the PASF/(Bmim) Cl solution is very different from that of PASF/DMAc solutions. In DMAc, as concentration increases viscosity increases, while the rheological behavior of the PASF/(Bmim) Cl solution exhibits a maximum in the viscosity‐concentration plots.     

Nature of dual fluorescence in 2-(quinolin-2-yl)-3-hydroxychromone: Tuning between concurrent H-bond directions and ESIPT pathways

Synthesis of the quinoline-substituted 3-hydroxychromone is reported, spectral and fluorescent properties of the title compound are investigated in different solvents. The question of the possibility of the participation of the substituent heterocycle’s nitrogen atom in H-bond formation as well as in the ESIPT process is discussed. Quantum-chemical modeling provides evidence that the structure with an alternative H-bond to nitrogen is more energetically favorable and strongly prevails in solutions. However, our calculations together with the experimental data reveal that the excited species with the intramolecular N…HO hydrogen bond type undergoes rapid radiationless deactivation. This leads to a conclusion that the low-intensity dual-band fluorescence of the title compound in solutions originates from the traces of the conformation with the traditional “flavonol-like” H-bond to the carbonyl oxygen atom. A possibility to reversibly tune the direction of the intramolecular H-bond formation and thus regulate the ESIPT process pathway is demonstrated by the example of protonation/deprotonation of the title compound in a methylene chloride solution.     

Optical properties of cyclometalated Pd(II) and Rh(III) complexes based on 2-(4-biphenylyl)-6-phenylbenzoxazole luminophore with ethylenediamine

Using the methods of electronic absorption and emission spectroscopy, we have studied the optical properties of cyclometalated [Pd(C??N)En]CH₃COO and [Rh(C??N)₂En]Cl complexes of 2-(4-biphenylyl)-6-phenylbenzoxazole luminophore with ethylenediamine. We have shown that, along with a bathochromic shift of intraligand spin-allowed ??-??* optical transitions by 1000?C1800 cm^?1, complexes are characterized by the occurrence of long-wavelength bands of a mixed nature (intraligand-metal-ligand charge transfer) in the range of 369??392 nm and by competing intraligand fluorescence (419?C423 nm) and phosphorescence (511?C532 nm) processes under low-temperature (77 K) photoexcitation.     

Intramolecular energy and charge transfer in 5-(9-anthryl)-3-(4-nitrophenyl)-1-phenyl-2-pyrazoline

The absorption and photoluminescence of the newly synthesized 5-(9-anthryl)-3-(4-nitrophenyl)-1-phenyl-2-pyrazoline (AN PP) were investigated. The absorption is the absorption of anthryl moiety at about 325-400 nm, superimposed on the broader absorption of 3-(4-nitrophenyl)-1-phenyl-2-pyrazoline moiety peaked at 420 nm. On excitation at 420 nm, the fluorescence spectrum has only one emission band from the pyrazoline moiety. This emission band exhibits a larger red shift with an increase in the polarity of solvents. But on excitation at 365 nm, the fluorescence spectrum has two emission bands coming from the anthryl and pyrazoline moieties, respectively. The intensity ratio of the two bands is different in solvents of different polarity. It is concluded that photo-induced intramolecular energy transfer from the anthryl to pyrazoline moiety exists simultaneously with the charge transfer from N (1) to C (3) in the pyrazoline moiety in the excited state and both compete with each other.     

Heats of solution and dilution for polyethylene oxide in several solvents

The Tian-Calvet microcalorimeter, as modified by Maron and Filisko, has been used to measure the heats of solution and dilution of a sample of polyethylene oxide (PEO) of M₂ = ca. 6000 in chloroform, methylene chloride, and water. By applying the Maron theory to these measurements, it was found from the organic solvent data that the heat of fusion of the PEO sample is 57.1 cal/g polymer, independent of the solution concentration or the solvent used. However, the solution behavior in water was different because PEO in organic solvents exists as a random coil, whereas in water its conformation is helical. By combining the water and organic solvent data, it can be shown that conversion of the random coils to the helix involves the evolution of 39.3 cal of heat per gram of polymer. This heat evolution accounts, in all probability, for the solubility of PEO in water.     

Theoretical insights into the formation of thiolate-protected nanoparticles from gold (III) chloride

Reaction pathways for the formation of thiolate-gold nanoparticles are investigated by density functional theory (DFT) and a new mechanism upon solvent polarity and tetraalkylammonium is obtained. In solvents with high polarities, [Au(I)SR]_n polymers can be formed as the precursor of metal ions prior to the addition of a reducing agent; while a product of [Cl…AuCl(HSR)] is identified as the precursor in solvents with low polarities, such as toluene and chloroform. In addition, tetraalkylammonium also has an obvious effect on the reactions when it is used as a phase transfer agent in the two-phase synthesis. These findings offer a systematic analysis on the pathways to thiolate-stabilized nanoparticles and give a favorable explanation by comparison with those in an experimental system.     

Electrospun cross linked rosin fibers

In this study, we describe the first reported preparation of rosin in fiber form through use of an electrospinning technique utilizing various solvent systems. The polymer concentration of the formed fiber was studied by using various solvents such as chloroform, ethanol, N-N dimethylformamide (DMF), tetrahydrofuran (THF), acetone, and methylene chloride (MC). An electrospray of the solution resulted in the beaded form of the rosin. By varying the polymer concentration with MC, we were then able to obtain uniform fibers. However, the fibers exhibited large diameter. We believe that it is possible to reduce the diameter of the rosin fibers through appropriate selection of electrospinning parameters. In addition, the morphological transitions from beads, to beaded fiber, to fiber were studied at different polymer concentrations. We propose a possible physical cross linking mechanism for the formation of rosin fibers during the electrospinning process. Our results demonstrate the feasibility of producing fiber nanostructures of rosin by using an electrospinning technique.