双8-羟基喹啉-席夫碱-锌高分子配合物的制备及发光性能

将5－甲酰基－8－羟基喹啉分别与对苯二胺、联苯二胺、4，4′－二氨基二苯砜反应，得到了三种双8－羟基喹啉－席夫碱配体，然后与锌离子配位，制得了一类新型的双8－羟基喹啉－席夫碱－锌高分子配合物。利用红外光谱、紫外可见光谱、元素分析对配体和配合物的结构进行了表征，利用荧光光谱研究了高分子配合物的光致发光性能。     

糠醛水杨酰腙锌（Ⅱ）和铅（Ⅱ）配合物的合成与光谱特性

由糠醛与水杨酰肼反应合成糠醛水杨酰腙席夫碱,然后再将其分别与过渡金属锌（Ⅱ）和铅（Ⅱ）作用合成两种新型的酰腙席夫碱配合物,并通过元素分析、紫外光谱、红外光谱等方法对所制备配合物进行表征。     

噻吩甲酰基吡唑啉酮缩β-丙氨酸配合物的合成、表征及极谱行为

在非水溶剂中 ,β 丙氨酸与 1 苯基 3 甲基 4 (2 噻吩甲酰基 )吡唑啉酮 5反应合成新型酰基吡唑啉酮席夫碱化合物 1 苯基 3 甲基 4 (2 噻吩甲酰基 )吡唑啉酮 5缩 β 丙氨酸 (HL) .通过回流席夫碱和金属硝酸盐合成了UO2 (Ⅱ )、Cu(Ⅱ )、Co(Ⅱ )和Fe(Ⅱ )金属配合物 .在乙酸 乙酸钠 (pH =4 .6 )缓冲溶液 饱和甘汞电极体系中 ,测量电位 - 1.2 4V处 ,测得铜配合物的极谱波 .元素分析及摩尔电导值表明 ,新配合物的组成为 [UO2 L2 ]·H2 O ,[CuL2 ]·2H2 O ,[CoL2 ]·2H2 O和 [FeL2 ]·2H2 O .运用红外光谱、紫外光谱、核磁共振谱、热谱和磁矩对配合物进行了表征 .结果表明 ,配合物的中心离子 (除UO2 2 + 以外 )均为 6配位 .铜配合物的Cu2 + 还原产生峰电流 ,其电极反应转移 1个电子 .     

钕、铽(Ⅲ)硝酸盐、水杨醛乙二胺双席夫碱、二甲亚砜三元配合物的NMR研究

用NMR的方法研究了新型稀土配合物:钕、铽(Ⅲ)硝酸盐与N,N-二亚水杨基乙二胺双席夫碱、二甲亚砜三元配合物的结构,并利用二维质子NOE谱和异核多量子相关谱完全归属了它们的质子和¹³C信号.     

酰基吡唑啉酮缩β-丙氨酸稀土配合物的合成与光谱表征

在非水溶剂中,β丙氨酸与苯甲酰基吡唑啉酮反应制备出新氨基酸席夫碱试剂:1苯基3甲基4苯甲酰基吡唑啉酮5缩β丙氨酸(HL)。通过回流席夫碱与稀土硝酸盐合成了10种稀土配合物。元素分析与摩尔电导值表明新配合物的组成为[REL2NO3](nH2O(RE=La,Sm,Eu,Tb,Y,n=2;RE=Pr,Ndn=1;RE=Dy,Er,Yb,n=3)。运用红外光谱、紫外光谱、核磁共振谱和荧光光谱对配合物进行了表征。结果表明席夫碱配体以3齿形式配位,RE3 的配位数为8。在可见光区522nm;573,584nm处分别发现Er和Nd配合物的超灵敏跃迁吸收峰。配合物的荧光光谱主要体现稀土离子的ff跃迁发光,配体的发光影响较小。配合物的荧光强度:ITb>ISm>IEu>IDy。     

新型双核锌(Ⅱ)大环席夫碱配合物的合成及谱学表征

由环腔孔径不同的大环席夫碱配体与醋酸锌反应合成了锌(Ⅱ)的双核席夫碱配合物.并用元素分析、核磁共振、红外光谱、质谱和紫外-可见光谱等方法对其结构和组成进行表征.     

新型大环席夫碱的合成及其荧光量子效率的研究

合成了单核席夫碱锌()配合物和系列大环双核席夫碱锌()配合物,研究了它们的荧光性能,并测定了它们的荧光量子效率。结果表明,大环席夫碱双锌配合物具有较强荧光效率,此类大环双核席夫碱化合物可以用于有机电致发光材料中。     

钕、铽(Ⅲ)硝酸盐、水杨醛乙二胺双席夫碱、二甲亚砜三元配合物的NMR研究

用NMR的方法研究了新型稀土配合物：钕、铽（Ⅲ）硝酸盐与N，N-二亚水杨基乙二胺双席夫碱、二甲亚砜三元配合物的结构，并利用二维质子NOE谱和异核多量子相关谱完全归属了它们的质子和13C信号．     

席夫碱稀土配合物与DNA的作用方式

以糠醛和对氨基苯磺酸反应合成席夫碱配体,与稀土离子配位制得相应的稀土配合物,并运用光谱法研究配合物与DNA之间的作用机制,为新型抗癌药物的设计开发提供依据。采用元素分析、红外和紫外光谱对配合物性质进行表征测试,确定其化学组成为REL(OH),RE为La~(3+)、Nd~(3+)、Eu~(3+),L为去质子形式的希夫碱配体。此外,运用光谱法和循环伏安法研究了REL(OH)配合物与鲱鱼精DNA之间的作用方式。配合物在加入DNA后,特征吸收峰强度发生明显的减色效应,但峰位红移不明显。配合物能够猝灭中性红-DNA体系的荧光。Fe(CN)_6~(3-)/~(4-)的氧化还原峰电流在配合物加入后减小,式量电位有正移趋势,表明配合物、Fe(CN)_6~(3-)/~(4-)与DNA的作用存在竞争。研究结果表明:这3种席夫碱稀土配合物与鲱鱼精DNA的作用均属于嵌插,且含有不同稀土离子的配合物与DNA的作用强弱不同,作用大小次序为Eu配合物La配合物Nd配合物席夫碱,这可能与DNA和配合物中的稀土离子所发生的作用有关。     

糠醛缩壳寡糖席夫碱及Cu(Ⅱ)配合物与DNA之间的作用机制

以糠醛和壳寡糖反应生成的席夫碱,与不同摩尔比的Cu2+配位合成配合物FCOS-Cu11、FCOS-Cu13和FCOS-Cu31,并研究配合物与DNA之间的作用机制。采用循环伏安、紫外-可见吸收光谱、粘度和DNA熔点测定的方法,分别研究了席夫碱及配合物与DNA之间的作用机制。合成的3种配合物具有电化学活性。加入DNA后,配合物的氧化峰电流减小,峰电位微弱移动。配合物的吸收峰强度减色显著,同时伴有峰位红移现象。配合物加入后,DNA的相对粘度和熔点呈增大趋势。结果表明,席夫碱及配合物与DNA之间存在嵌插结合,且3种配合物中的Cu2+含量与DNA的嵌插作用强度有关,结合强度依次为FCOS-Cu11FCOS-Cu13FCOS-Cu31。     

Experimental and Theoretical Study of the Electronic States and Spectra of TeH and TeLi

Gas-phase emission spectra of the hitherto unknown free radical TeLi have been measured in the NIR range with a Fourier-transform spectrometer. The emissions were observed from a fast flow system in which tellurium vapor in argon carrier gas was passed through a microwave discharge and mixed with lithium vapor in an observation tube. Two systems of blue-degraded bands were measured at high spectral resolution in the ranges 8000-9000 and 5700-6700 cm(-1) and vibrational and rotational analyses were performed. In order to aid in the analysis of the experimental data, a series of relativistic configuration interaction calculations has been carried out to obtain potential curves for the low-lying states of TeLi and the isovalent TeH and also electric dipole transition moments connecting them. As in the TeH system, the ground state of TeLi is found to be X(2)Pi(i), but with a remarkably smaller spin-orbit splitting. The TeLi calculations indicate a strongly bound A(2)Sigma(+) state, while in TeH the analogous state is computed to lie significantly higher at approximately 32 000 cm(-1), and it is strongly predissociated. Based on the theoretical analysis, the observed TeLi band systems are assigned to the transitions A(2)Sigma(+)(A1/2)-->X(1)(2)Pi(3/2)(X(1)3/2) and A(2)Sigma(+)(A1/2)-->X(2)(2)Pi(1/2)(X(2)1/2). Analysis of the spectra has yielded the molecular constants (in cm(-1)) X(1)(2)Pi(3/2):omega(e)=457.49(3), omega(e)x(e)=2.482(9), B(0)=0.408908(8); X(2)(2)Pi(1/2): T(e)=2353.44(3), omega(e)=456.28(4), omega(e)x(e)=2.635(8), B(0)=0.414954(8), p(0)=1.00637(4); A(2)Sigma(+): T(e)=8574.64(2), omega(e)=437.81(3), omega(e)x(e)=2.581(8), B(0)=0.423903(8), p(0)=-0.19915(2), where the numbers in parentheses are the standard deviations of the parameters. Comparison of the isovalent TeLi and TeH systems emphasizes that the difference in bonding character (ionic in TeLi vs covalent in TeH) is responsible for qualitative differences in the electronic spectra of these two molecules. Copyright 2001 Academic Press.     

Geometry and Elasticity of Strips and Flowers

We solve several problems that involve imposing metrics on surfaces. The problem of a strip with a linear metric gradient is formulated in terms of a Lagrangian similar to those used for spin systems. We are able to show that the low energy state of long strips is a twisted helical state like a telephone cord. We then extend the techniques used in this solution to two–dimensional sheets with more general metrics. We find evolution equations and show that when they are not singular, a surface is determined by knowledge of its metric, and the shape of the surface along one line. Finally, we provide numerical evidence by minimizing a suitable energy functional that once these evolution equations become singular, either the surface is not differentiable, or else the metric deviates from the target metric.     

Synthesis and characterizations of hollow spheres and nanospheres of Au

Hollow spheres and nanospheres of Au have been prepared by a simple reaction of HAuCl₄·4H₂O, NaOH and (NH₂OH)₂·H₂SO₄ in the presence of gelatin. The role of gelatin and the effect of the temperature of the reaction in producing the spherical particles of Au are discussed. The products were characterized by powder X-ray diffraction (XRD), transmission electron microscopy and UV–Vis absorption spectroscopy. The sizes of the nanospheres of Au were estimated by the Debye–Scherrer formula according to the XRD spectrum. PACS  81.05.Bx; 81.05.Rm; 81.07.-b; 81.16.Be; 81.20.Fw     

Topological dislocation-type defects and mechanisms of plasticity and failure of nanostructured and amorphous materials

Possible mechanisms of plastic deformation and failure of nanostructured and cluster amorphous materials have been considered. It is shown that the most probable carriers of plastic deformation in these materials are macrodislocations—linear topological defects of the regular nanocrystallite packing in the nanostructure or cluster packing in amorphous materials. Continuum models are proposed to describe the processes of plastic deformation and failure of nanostructured and cluster amorphous materials. Original Russian Text ? L.S. Vasil’ev, S.F. Lomaeva, 2009, published in Izvestiya Rossiiskoi Akademii Nauk. Seriya Fizicheskaya, 2009, Vol. 73, No. 1, pp. 128–131.     

NOx formation and flame velocity profiles of iso- and n-isomers of butane and butanol

NO formation and flame propagation are studied in premixed flames of iso- and n-isomers of butane and butanol through experimental measurements and direct simulation of experimental profiles. The stabilized flame is realized through the impingement of a premixed combustible jet from a contraction nozzle against a temperature-controlled plate. The velocity field is obtained by means of Particle Image Velocimetry (PIV) and nitric oxide concentration profiles are measured using Planar Laser Induced Fluorescence (PLIF), calibrated using known NO seeding levels. It is found that NO formation in n- and iso-isomers is comparable under the conditions considered, except for rich butanol mixtures, whereby NO formation is higher for iso-butanol. Generally, less NO is formed in butanol flames than in the butane flames. The experiment is simulated by a 1D chemically reacting stagnation flow model, using literature models of C1–C4 hydrocarbons [Wang et al., 2010] and butanol combustion chemistry [Sarathy et al., 2009, 2012]. NO prediction is tested using two of these mechanisms with a previously-published NO_x submechanism added into the butane and butanol models. While a good level of agreement is observed in the velocity field prediction under lean and stoichiometric conditions, discrepancies exist under rich conditions. Greater discrepancies are observed in NO prediction, except for the C1–C4 mechanism which shows good agreement with the experiment under lean and stoichiometric conditions. The current study provides data for further development of mechanisms with NO_x prediction capabilities for the fuels considered here.     

Quantum and surface properties of free films and nanoshells of molecular and atomic thicknesses

An original technology and the properties of new thin film nanoobjects, free films and shells of molecular and atomic thicknesses, are presented. Special attention is paid to shells of monoatomic or monomoleculer thickness with unique surface properties that have not been found in bulk materials.     

ORSAT and modifications of SEFT and APT

Up to now, three subspectra are usually needed for the complete assignment of all signals in 13C spectrum: two DEPT spectra (phi = 90 degrees and phi = 135 degrees) and a proton decoupled spectrum. In this paper, we present a method in which a complete assignment becomes possible with merely two spectra. For this purpose, a new pulse sequence (ORSAT) has been elaborated by using off-resonance irradiation. The method described here is a further development of SEFT and APT. The second required spectrum is a DEPT (phi = 135 degrees). Signal assignment of cholesteryl acetate is demonstrated as an example. 13C routine spectroscopy can be significantly accelerated by applying this method.     

Absorption and luminescence of amino- and benzoylaminoanthraquinones

Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 53, No. 3, pp. 396–402, September, 1990.     

受控核聚变两大途径的对比与结合

目前人们探索受控核聚变主要是从两个方向着手：磁约束受控核聚变和惯性约束受控核聚变，但目前还无法判定到底哪一种途径更为可取，文章首先对这两种途径进行对比，指出各自的特点和困难，在此基础上提出了一种结构相对简单，成本相对较低的三轴六极磁镜系统设想，希望能将磁约束和惯性约束和惯性约束结合起来，以实现受控核聚变反应。