CaCO3粉末表面光聚合处理的研究

采用表面光聚合技术处理CaCO₃粉末,研究了反应温度、时间、单体浓度等对丙烯酰胺(AAM)在CaCO₃粉末表面光聚合的影响,并采用X光电子能谱(ESCA)、粒度分析、扫描电子显微镜(SEM)和模型模拟分析等研究了表面光聚合处理碳酸钙(CaCO₃)的结构.结果表明:紫外光能有效地引发AAM在CaCO₃粒子表面聚合.经光聚合处理后,CaCO₃粒子表面形成了聚丙烯酰胺(PAAM)包覆层,该包覆层与CaCO₃粒子结合紧密,不能被溶剂洗涤清除.光聚合处理后CaCO₃粒子表面较光滑,分散性可得到提高,CaCO₃粒子粒径增大.     

两种紫外-真空紫外光谱辐射标准的比对

研究了紫外 真空紫外波段壁稳氩弧光谱辐射标准光源及基于同步辐射标准的传递标准光源———氘灯的光谱辐射特性 ,建立了高精度光谱辐射计量系统 ,在 16 5～ 30 0nm之间 ,将两种类型光谱辐射标准进行比对 ,相对光谱分布的一致性好于± 5 %。     

人工神经网络紫外分光光度法同时测定去痛片组分含量

用BP人神经网络处理复方制剂去痛片的紫外吸收光谱数据,达到了对其各组分含量进行同时测定的目的。通过对网络结构和参数的优化,提高了预报的准确度。     

Laser-induced fluorescence measurements of a 3 Π metastable carbon monoxide in a high enthalpy flow

Excitation of carbon monoxide molecules has been carried out in a cold cell and in a low-pressure plasma jet using an ArF narrow-band excimer laser. The different excitation models are discussed and the relevance of atomic carbon absorption into the laser cavities is pointed out. Excitation spectra of Cameron bands have been obtained in a room-temperature cell and compared with calculated spectra. A value of the constant σ related to the interaction strength between a ³ Π( v = 2) state and its neighbouring singlet states is derived: 0≤σ≤0.05. The fluorescence spectrum following broad band excitation of CO has been observed both in UV and visible. Similar experiments carried out in a high enthalpy flow have allowed to point out the presence of a ³ Π metastable carbon monoxide. A method for relative measurements of this species concentration is proposed. Received 9 April 2001 and Received in final form 13 June 2001     

On the Stark broadening of the He I 447.1 nm spectral line

Characteristics of the Stark broadened and overlapping 447.1 nm He I spectral line and its forbidden 447.0 nm components have been measured at electron densities between 4.4×10²² m^-3 and 8.2×10²² m^-3 and electron temperatures between 18 000 K and 33 000 K in plasmas created in five various discharge conditions using the low pressure pulsed arc as an optically thin plasma source operated in helium-nitrogen-oxygen gas mixture. Good agreement was found among our measured line characteristics and their existing calculated values, based on the quasistatic approximation. Possible influence of the singly ionized oxygen impurity atoms (O II) on the intensity values of the dip between allowed and forbidden components was found that can explain the disagreement among some existing experimental and calculated line characteristics data, at higher electron temperatures and densities. On the basis of the observed asymmetry of the 447.1 nm spectral line profile we have obtained the ion contribution parameter at 10²² m^-3 electron density and 8 000 K electron temperature. Received 20 February 2001 and Received in final form 25 April 2001     

Ultraviolet photoelectron spectroscopy of Si 4 - to Si 1000 -

Using a new experimental setup we have measured UV (h ν = 6.4 eV) photoelectron spectra of cold silicon cluster anions Si _n ^- in a very broad size range. For sizes up to n = 46 the spectra exhibit rich structures. For larger sizes only smooth spectra have been obtained. No trace of a bandgap has been found even for clusters with more than 1000 atoms. Received 30 November 2000     

Semi-classical analysis of helium broadened acetylene (ν 1 +3ν 3 ) band transitions measured by a NIR diode laser spectrometer

An inversion method for ion Doppler shift of spectrum lines was developed for plasma velocity measurements. By reducing the problem to the vectorial Radon transform, the characteristics of plasma ion velocity distribution such as vector potential/vorticity and velocity components were computed in two-dimensional space. Computer simulation of the reconstruction of different vector potential (vector field) models gives evidence that the reconstruction errors are acceptable, and the method can surely be used for real experimental data. Received 10 March 2001 and Received in final form 25 July 2001     

Electron temperature measurement in a surface-wave-produced argon plasma at intermediate pressures

The main objective of this work is to obtain the electron temperature in an argon surface-wave-produced plasma column at intermediate gas pressures. After proving that argon upper excited states remain in Excitation Saturation Balance, the value of electron temperature along the plasma column has been obtained using a modified Saha equation and a corrected Boltzmann-plot. Moreover, the electron energy distribution function has been verified to be nearly Maxwellian in a 0.8-2.8 torr intermediate pressure range. Received 24 July 2000 and Received in final form 19 January 2001     

NaGdF_4:Eu~(3 )的结构和VUV荧光性质

利用水热方法合成了纯度较高的六方结构的 NaGdF4,在氧气存在条件下 950℃加热处理可以使其转变为 CaF2型立方结构。在真空紫外光激发下,六方结构的 NaGdF4∶ Eu3＋中的 Gd3＋离子吸收一个光子,并将能量分两步传递给 Eu3＋离子,发生双光子发射。立方结构的 NaGdF4∶ Eu3＋中存在有一定量的氧离子取代缺陷,使 Gd3＋离子 4f-5d跃迁移到 177nm附近,这与惰性气体放电产生的真空紫外光波长一致。     

Selective determination of total normal microcystin by colorimetry, LC/UV detection and/or LC/MS

Microcystins, hepatotoxic cyclic heptapeptides, are produced by freshwater cyanobacteria, and are classified four groups according to the amino acid structure at unit 7. Normal microcystins contain N-methyldehydroalanine (Mdha) or dehydroalanine (Dha) at unit 7, and command the great part of all microcystins. As unusual microcystin classes, [Dhb⁷]microcystins, [ - and -Ala⁷, or N-MeAla⁷]microcystins and [ -Ser⁷]microcystins have been found.

On tumor initiation and/or promotion activities of microcystins, the tumor promotion activity of normal microcystins has been found, but cancer-related activities of microcystins belonging in the other classes have not been clear.

To determine normal microcystins as hepatotoxic tumor promoters, a selective determination method was developed. Only Mdha or Dha in normal microcystins was reacted with glutathione (GSH). The GSH-normal microcystins conjugates were reacted with trinitrobenzene sulfonate (TNBS). The TNB–GSH-normal microcystin conjugate can be determined as the total normal microcystin by colorimetry. After methanolysis of the conjugate, dimethyl TNB–glutamate from the conjugate was determined by liquid chromatography/ultraviolet detection (LC/UV) and/or liquid chromatography/mass spectrometry (LC/MS). The detection limits of the total normal microcystin by colorimetry, LC/UV and/or LC/MS were 1 μg, 10 and 0.1 ng, respectively.