离子色谱法测定芳香族聚酰胺纤维中硫、钠、钾、钙、镁

应用离子色谱法(IC)测定芳香族聚酰胺纤维中硫、钠、钾、镁及钙。测定阴离子时,试样置于铂坩埚中用艾斯卡试剂覆盖,置于马弗炉中,450℃灼烧1 h使有机物碳化,取出,稍冷,再加少许艾斯卡试剂,升温至850℃灼烧1．5 h,使有机物完全分解。坩埚中的熔块经冷却后用去离子水浸出,用18 mmol·L-1碳酸钠及17 mmol·L-1碳酸氢钠混合溶液定容后,用IC法的阴离子方式测定。用IC法测定阳离子时,试样置于铂坩埚中,不必加艾斯卡试剂,置于马弗炉直接灼烧至有机物完全分解。残渣用1 mol·L-1硝酸或1 mol·L-1盐酸超声波处理,用去离子水洗涤坩埚并定容至100 mL,按所测得峰面积值从标准曲线查得其含量。用此方法测定SO42-,Na+,K+,Mg2+及 Ca2+的检出限依次为0．02,0．25,0．25,0．70及0．80 mg·L-1。     

一种高灵敏的压电免疫传感器用于高密度脂蛋白的测定

采用自组装单层膜(SAMs)技术在压电石英晶体的金电极表面组装巯基丙酸SAMs,以盐酸1-乙基-3-(3-二甲基氨基丙基)碳二亚胺(EDC)和N-羟基琥珀酰亚胺(NHS)作偶联剂,以共价键合方式固定高密度脂蛋白抗体,研制成一种高灵敏的压电免疫传感器用于检测人血清中低含量的高密度脂蛋白。利用压电装置的实时监测功能,考察了巯基丙酸在金电极表面的自组装成膜过程与机制;研究了晶振固定抗体及其反应结合抗原的液相振荡行为和传感特性。传感器采用初始速率法测定高密度脂蛋白的线性浓度范围为1.63~18.8 mg.L-1,检出限为0.82 mg.L-1。     

膜载体酶标记dip-stick快速检测西维因的痕量残留

利用直接竞争酶联免疫吸附分析技术研发了一种快速、灵敏的膜载体酶标记dip-stick农残西维因检测方法。该方法以带正电尼龙膜(Millipore)为固相载体,将西维因抗体包被于膜上,包被有抗体的膜插入含有西维因和西维因酶标抗原的混合液中竞争反应10 min后直接目视判断分析结果。该方法的整个检测过程只需15 min,对西维因的检出限可达到10μg.L-1,且稳定性较好。通过与高效液相色谱法(HPLC)比较,验证了该检测方法的有效性,可作为品质控制和快速定性检测的一种有效工具。     

全谱直读ICP-AES法测定纺织品中重金属总量

采用干法灰化法处理纺织品样品,以全谱直读ICP-AES法对纺织品中铅、镉、砷、铜、钴、镍、铬、锑等重金属元素进行同时测定。方法的相对标准偏差为1.56％～9．62％,各元素的加标回收率为83．2％～108.4％。该方法准确、可靠,完全可以满足日常检测的需要。     

七(2,3-二-O-乙酰基-6-O-叔丁基二甲基硅烷基)-β-环糊精毛细管色谱柱的研制及色谱性能

合成了七（2,3-二-O-乙酰基-6-O-叔丁基二甲基硅烷基）-β-环糊精,并采用静态法成功地将其涂渍到弹性石英毛细管柱上。研究了其气相色谱分离性能,发现此固定相涂渍性好,柱效较高,热稳定性好,对卤代芳烃异构体以及难分离的二取代苯的位置异构体具有良好的分离能力。     

聚氯乙烯膜碘离子选择电极在溴碘离子共存体系分析中的应用

介绍了聚氯乙烯膜碘离子选择电极(PVC-I-ISE)的制备方法,电极对碘离子的能斯特响应斜率为59 mV/pI,响应的线性范围为4.0×10-5~1.0×10-2mol.L-1,检出限为1.6×10-5mol.L-1,低于用银ISE的检出限,电极的使用寿命为一个月以上。将制备的碘离子选择电极作为指示电极用于对溴、碘混合离子体系进行连续分别电位滴定,并与以银电极为指示电极的电位滴定方法进行了比较。结果表明用PVC-I--ISE作指示电极,可在I--Br-共存的混合溶液中进行两离子的连续电位滴定,而用银-ISE时则不能。     

Self-organized Criticality in an Earthquake Model on Random Network

A simplified Olami-Feder-Christensen model on a random network has been studied. We propose a new toppling rule — when there is an unstable site toppling, the energy of the site is redistributed to its nearest neighbors randomly not averagely. The simulation results indicate that the model displays self-organized criticality when the system is conservative, and the avalanche size probability distribution of the system obeys finite size scaling. When the system is nonconservative, the model does not display scaling behavior. Simulation results of our model with different nearest neighbors q is also compared, which indicates that the spatial topology does not alter the critical behavior of the system.     

New Matrix Lie Algebra, a Powerful Tool for Constructing Multi-component C-KdV Equation Hierarchy

A set of new multi-component matrix Lie algebra is constructed, which is devoted to obtaining a new loop algebra A-2M. It follows that an isospectral problem is established. By making use of Tu scheme, a Liouville integrable multi-component hierarchy of soliton equations is generated, which possesses the multi-component Hamiltonian structures. As its reduction cases, the multi-component C-KdV hierarchy is given. Finally, the multi-component integrable coupling system of C-KdV hierarchy is presented through enlarging matrix spectral problem.     

Scheme for Quantum Entanglement Swapping on Cavity QED System

We propose a scheme for realizing quantum entanglement swapping between the atoms in cavity QED. With only virtual excitation of the cavity during the interaction between the atoms and cavity, the scheme is insensitive to the cavity mode states and the cavity decay. The ideas can also be utilized for realizing entanglement swapping between the atomic levels in a single atom and the atomic levels in the Bell states and between the atomic levels in the Bell states and the atomic levels in the W states.     

Quantum Inequality Bounds for Free Rarita-Schwinger Field in Flat Spacetime

Although quantum field theory allows the local energy density negative, it also places severe restrictions on the negative energy. One of the restrictions is the quantum energy inequality (QEI), in which the energy density is averaged over time, or space, or over space and time. By now temporal QEIs have been established for various quantum fields, but less work has been done for the spacetime quantum energy inequality. In this paper we deal with the free Rarita-Schwinger field and present a quantum inequality bound on the energy density averaged over space and time.Comparison with the QEI for the Rarita-Schwinger field shows that the lower bound is the same with the QEI. At the same time, we find the quantum inequality for the Rarita-Schwinger field is weaker than those for the scalar and Dirac fields. This fact gives further support to the conjecture that the more freedom the field has, the more easily the field displays negative energy density and the weaker the quantum inequality becomes.