锰、铑原卟啉IX-二甲酯配合物共振拉曼光谱研究

合成了MnPPCl,RhPPCl,RhPPN3,RhPP(CO)Cl四种配合物 (PP =ProtophyrinIXDimethy1Ester) ,用元素分析、红外吸收光谱及紫外吸收光谱确定了配合物的组成 ,测定了它们的共振拉曼光谱 ,对特征谱带进行了归属。分析了拉曼谱带和电子吸收谱带变化的原因 ,提出了谱带频率的变化受金属离子外层d电子和轴配体的影响。     

铕离子探针研究Al2O3的相变过程

氧化铝具有许多重要的工业用途，而制备高热稳定活性氧化铝的技术也在不断地发展[1，2]，因此，研究其高温烧结下的相变过程很有意义．离子深法作为新型测试手段，已成功地用于生物大分子结构与功能研究方面［‘］，而在固体材料测试中的应用尚未见报道．我们以EU’“作为荧光探针，并结合＊＊D和＊nR研究了川对。在不同烧结温度下的相变过程．1实验部分样品的制备采用复盐分解法．先将Elf刀s用高纯硝酸溶解定容．以占AlzO。重量1％的量加入到硫酸铝锭溶液中，进行超声处理，冷冻干燥．再依次登于900”C、1000C、1100C、1200C的高温炉…     

若干1-(N-甲基-4-吡啶鎓基)-3-(N-甲基-4-吡啶亚基)-4-烷基环戊烯-1-酮-5菁化合物可见吸收光谱的溶剂效应

菁是一类很重要的离子型染料和感光材料,也有极少数可用作激光染料,绝大部价菁染料为直链分子。我们最近合成了一系列带有五员桥环的菁,并研究了这些桥环菁化合物的质子化平衡和荧光性质。     

CTAB胶束微环境中BY增溶位置的探讨

本文用ＵＶ吸收光谱对（ＢＹ＝ＣＴＡＢ）体系胶束化过程中预胶束的形成，以及预胶束向胶束的转变过程进行了分析。采用Ｇｏｕｙ－Ｃｈａｐｍａｎ模型，建立了ＣＴＡＢ胶束微环境中ＢＹ表现解离常数与胶束结构参数之间的定量关系，根据水溶液和各种盐浓度条件下ＣＴＡＢ胶束溶液中酸碱解离常数的测量，分析了ＢＹ在ＣＴＡＢ胶束扩散层中的增溶位置，讨论了ＣＴＡＢ胶束对ＢＹ选择性吸附的特性。     

有机镓配合物的合成及其质谱

本文通过三环戊基镓与取代苯酚, 有机酸, 氨基酸反应合成了八个新的有机镓配合物, 这些配合物经过元素分析、质谱、核磁共振或红外光谱鉴定; 质谱研究表明这些配合物均以二聚体的形式存在。     

铁／锌催化剂的物相结构及其还原行为的穆斯堡尔谱研究

以Mossbauer谱为手段,研究了用于F-T合成的Fe/Zn催化剂的物相结构,并考察了组成及制备方法的影响,同时还对其还原、碳化行为进行了探讨.发现锌对铁的还原有抑制作用,它能够稳定二价铁不被进一步还原.研究还表明,我们所研制的Fe/Zn催化剂是一种高分散度的铁锌化合物,室温下具有超顺磁特性.     

二碘化铕的相变结构及荧光性质

本文用ＤＴＡ、Ｘ－ｒａｙ粉末衍射和荧光光度计等方法研究了ＥｕＩ２的相变和结构及荧光性质，用退火和淬火的方法得到了ＥｕＩ２的三种不同结构，并在荧光光谱上有不同的反映，首次发现ＥｕＩ２的低温变体，ＥｕＩ２－Ⅲ，正交晶系，空间群为ｐｎｍａ，ａ＝１．２２８７ｎｍ，ｂ＝０．４８８７ｎｍ，ｃ＝０．８３８４ｎｍ，Ｚ＝４。     

An Infrared Spectroscopic Study on the Hofmann- and en-Td-type Clathrates: Mn(NH3)2Zn(CN)4 .2benzene and Mn(ethylenediamine)Zn(CN)4.2benzene

Infrared spectra of Mn(NH₃)₂Zn(CN)₄.2C₆H₆ andMn(ethylenediamine)Zn(CN)₄.2C₆H₆ are reported. The spectral data suggest that these compounds are similar in structure toHofmann-T_d-type and the en-T_d-type clathrates,respectively. There is good evidence for H-bonding from ammoniaN–H to benzene as a to H-bond.     

A neuro-fuzzy system for X-ray spectra interpretation

A decision scheme for the interpretation of spectra from wavelength dispersive X-ray fluorescence spectrometry is described that encompasses elements from three areas of artificial intelligence: fuzzy logic, rule based expert systems and neural net technology.After transforming the recorded spectra to line spectra by appropriate background correction a reasoning scheme is applied that takes into account not only the observed spectra, but also the recording conditions and prior spectroscopic information regarding the relative emission probabilities and the usefulness of the different lines for the purpose of element identification. The latter is done on the basis of a previously described scheme to compute conditional a posteriori Bayes probabilities for a mean matrix. These different pieces of information are then assembled into a battery of fuzzy rules. The importance of the rules as well as the importance of the X-ray lines is determined in a training process, similar to the one in a feedforward back-propagation network.To further stabilize the results this network is pruned in a second training cycle. This, however, had little effect on the quality of interpretation.The advantages of this approach to the interpretation of X-ray spectra over older ones are numerous: the system adapts itself to better interpret spectra that are of greater importance to a laboratory as these are better represented in the training set; the fuzzy logic is capable of working with incomplete and uncertain knowledge, and the neural network results based on these fuzzy rules is readily interpretable by the X-ray spectroscopist as every rule can be expressed also in natural language as in any classical rule based system.On leave from Silesian University, Katowice, Poland     

Comparison of the Dynamics of Water Molecules in Crystals of Proton-Ordered Ice IX and Its Proton-Disordered Analog III

A computer simulation of proton-ordered ice IX and its proton-disordered analog III (768 molecules, 90 K) was carried out by the molecular dynamics method using Poltev–Malenkov's potential. For ice IX, the differences in the dynamic characteristics of molecules with O(1) and O(2) are much wider than those in the case of ice III. The libration spectrum of ice IX has a number of distinct acute peaks, and the spectrum of ice III is strongly smoothed. These peculiarities are explained by the proton ordering of ice IX and disordering of ice III. The latter is responsible for the great differences in the short- and especially long-range environment of water molecules in ice crystals and hence for the presence of many molecules with different dynamic characteristics. Thus averaging over a large number of different vibrational spectra of molecules leads to a smoothed total spectrum in the case of the proton-disordered crystal modification of ice.