T(2,2,n) U (U Ci)的匹配等价图类i∈A

利用图的匹配多项式及其最大实数根的性质完整刻画了T(2,2,n)U(U C<,t>)(n≥3,A是大于等于3的整数组成的可重集)的匹配等价图类.     

一维Burgers方程和KdV方程的广义有限谱方法

给出了高精度的广义有限谱方法．为使方法在时间离散方面保持高精度,采用了Adams-Bashforth 预报格式和Adams-Moulton校正格式,为了避免由Korteweg-de Vries(KdV)方程的弥散项引起的数值振荡, 给出了两种数值稳定器．以Legendre多项式、Chebyshev多项式和Hermite多项式为基函数作为例子,给出的方法与具有分析解的Burgers方程的非线性对流扩散问题和KdV方程的单孤独波和双孤独波传播问题进行了比较,结果非常吻合．     

邻二氮菲荧光法测定氯碱厂阳极泥中痕量钌

研究了在乙酸-乙酸钠缓冲溶液中,在盐酸羟胺还原剂存在下,于水浴中加热近沸,保温5 min,钌与邻二氮菲形成1∶3络合物。它的荧光激发波长峰为448 nm,发射波长峰为586 nm。钌与荧光强度线性范围为0～10μg·(25 mL)-1。样品中的钌通过蒸馏分离,方法应用于氯碱厂阳极泥中钌的含量分析,具有满意的分析结果。     

东北地区三种鸟的繁殖特征与蛋壳微量元素的关系

采用火焰原子吸收方法,对栗斑腹鹀、大山雀、[树] 麻雀蛋壳中微量元素含量及其与繁殖特征之间的关系进行了研究。对五种微量元素的仪器工作条件进行了优化,并证实五种元素之间无干扰。加标回收率实验表明Mn, Mg, Cu, Fe和Zn五种元素回收率均在95%～104%之间,表明此方法具有较高的准确度。微量元素测定表明栗斑腹鹀蛋壳Zn和Mn元素的含量均大于大山雀和[树] 麻雀,但Cu,Fe和Mg含量均小于大山雀和[树] 麻雀。栗斑腹鹀的繁殖成功率和繁殖成活率最低,[树] 麻雀的繁殖成功率和繁殖成活率最高,大山雀居中。方差分析表明,栗斑腹鹀、大山雀和[树] 麻雀的五种微量元素含量、繁殖成功率和繁殖成活率均达到显著或极显著差异。相关分析表明,三种鸟繁殖成功率和繁殖成活率与Zn和Mn含量之间达到显著或极显著负相关,表明栗斑腹鹀、大山雀、[树] 麻雀繁殖特性受到蛋壳微量元素Zn和Mn的影响。栗斑腹鹀蛋壳Mg,Cu和Fe含量低,影响其幼鸟在蛋壳内的生长发育,导致极低的繁殖成功率。     

Scheme for Implementing Assisted Cloning of an Unknown d-Dimension Equatorial Quantum State by Remote State Preparation

In this paper, we propose a protocol that can produce perfect copy of an unknown d-dimensional equatorial quantum state with assistance from a state preparer. In this protocol, the maximally and non-maximally entangled bipartite d-dimensional of states are used as the quantum channels, respectively. The first stage of the protocol requires usual teleportation. In the second stage of the protocol, with the assistance of the preparer, the perfect copy of an original unknown state can be produced.     

表面修饰纳米碳管复合二氧化硅凝胶玻璃的制备研究

采用羧基化、酰氯化和酰胺化等三步化学反应实现了r-氨基丙基三乙氧基硅烷(NH₂(CH₂)₃Si(OC₂H₅)₃,APTES)对纳米碳管(CNTs)的表面修饰。在此基础上,采用溶胶-凝胶工艺将其引入到二氧化硅凝胶玻璃中,并通过红外IR光谱、扫描电子显微镜SEM分析测试方法对所得样品的组成和结构进行表征。结果表明,经过一系列的化学处理,成功实现了CNTs与APTES的共价键合而达到表面修饰的效果。溶胶-凝胶过程中,先驱液中正硅酸乙酯(Si(OC₂H₅)₄,TEOS)、r-缩水甘油醚基丙基三甲氧基硅烷(CH₂OCHCH₂O(CH2)₃Si(OCH₃)₃,GPTMS)、CNTs-APTES分别发生水解,并经过共同聚合反应形成二氧化硅三维网络结构,而CNTs也借助于APTES而被化学键合到二氧化硅网络中,实现了在二氧化硅凝胶玻璃基质中的均匀分散,从根本上克服了CNTs在固相基质中团聚的问题。     

Darboux Transformation and Soliton Solutions for InhomogeneousCoupled Nonlinear Schrödinger Equations with Symbolic Computation

With the aid of computation, we consider the variable-coefficient coupled nonlinear Schrödinger equations with the effects of group-velocity dispersion, self-phase modulation and cross-phase modulation, which have potential applications in the long-distance communication of two-pulse propagation in inhomogeneous optical fibers. Based on the obtained nonisospectral linear eigenvalue problems (i.e. Lax pair), we construct the Darboux transformation for such a model to derive the optical soliton solutions. In addition, through the one- and two-soliton-like solutions, we graphically discuss the features ofpicosecond solitons in inhomogeneous optical fibers.     

超重核研究谱仪的RFQ冷却聚束器RFQ1L

介绍了超重核研究谱仪中RFQ冷却聚束器RFQ1L的结构和运用SIMION程序对离子的冷却、聚束、引出和撇气过程的模拟情况。 模拟显示: 通过仔细选择工作点就完全可以把经过充气反冲质量分离器分离后的低品质束流转化为斑点小、发射度小和能量单一的高品质束流, 为紧接其后的磁铁和激光高效率分析提供条件。The structure and the simulation results about the cooling,bunching,extraction and skimming of the RFQ cooler and buncher RFQ1L, which is an important part of the being built super heavy nuclide research spectrometer, have been introduced. It shows that, by careful choice of its working point, we can obtain an ion beam with small beam spot, small emittance and mono energy, which can satisfy the requirements of the successive analyses by dipole and laser with high efficiencies.     

二苯并18冠6促进钾离子在微液-液界面上的迁移反应

本文研制出一种用于构造互不相溶电解质界面 (ITIES)的两亲性微孔电极 ,并对发生于该界面上的二苯并 18冠 6 (DB18C6 )促进钾离子的迁移反应进行了研究 ,计算其相关的反应参数 .实验证明 ,该方法操作简便 ,是研究ITIES界面上电荷迁移反应的一种有效工具     

厚透镜近似下激光驻波场中原子动力学研究

研究了在厚透镜近似下 ,原子在激光驻波场中的动力学行为 .通过直接演化一维薛定谔方程 ,发现当激光的强度较大时 ,原子束将会聚焦形成几个焦点 .如果激光的强度更大 ,驻波场中的原子将会出现一种“隧道”现象 ,此时 ,原子受一些实验参数 (如焦平面位置、激光强度等 )的影响程度将大大降低 .这种现象有利于提高原子在驻波场中聚焦沉积的效果 . The dynamics of atoms in laser standing wave (SW) in the regime of over-focused immersion-lens is studied. Through directly evolving a one-dimensional Schrdinger equation, we find that multiple focusing appears when laser intensity is larger than that required for simple focusing. If laser intensity is much higher than that for the single focusing, a "channeling" phenomenon appears, which is insensitive to the variation of some parameters, such as focal plane position and laser intensity...