The change of the superstructure of semicrystalline polymers during deformation: results from small-angle scattering with synchrotron radiation

The change of the superstructure of different polyethylenes during uniaxial deformation is investigated. The method used is small-angle scattering with synchrotron radiation. For branched polyethylene (Lupolen 1840D) the whole deformation range is analyzed. Beginning with superstructure of the lamellar cluster type, the superstructure partly disappears on a time scale of a few minutes and the fibrillar structure is built up. The degree of destruction and rebuilding depends on the drawing temperature. For very high molecular weight polyethylene (GUR) a reversible change of the superstructure at higher deformation ratios and at different temperatures is observed. The superstructure of (ethylene—hexene) copolymers (TIPELIN) at high draw ratios depends on the drawing temperature and is almost independent of the side group content. Interfibrillar microcracks parallel to the draw direction are produced in samples with a low side group content for draw ratios λ ≥ 1.5.     

一种新颖的超结构光纤Bragg光栅梳状滤波器的设计

报道一种新颖的用于多波长光纤激光器的超结构光纤Bragg光栅（SFBG）梳状滤波器，其突出特点是仅由单个光栅构成、折射率调制和局部啁啾富于变化、反射峰均匀性好、窄带宽和标准的信道间隔.采用基于LP算法的IS光纤光栅设计技术，将整体加窗切趾法改进为各信道独立加窗切趾，成功地设计出所需的SFBG，同时对SFBG的制作技术也进行了探讨.用传输矩阵法分析反射谱、时延曲线和群时延抖动.结果表明，所设计的SFBG满足各项设计指标要求，在DWDM系统中，这种新颖的SFBG可望成为用于多波长光纤激光器的最理想的高性 能梳 关键词： 超结构光纤Bragg光栅 光栅设计 梳状滤波器     

Mixed crystals in the system Cu2MnGexSn1−xS4: Phase analytical investigations and inspection of tetrahedra volumes

Cu₂MnGeS₄ crystallizes orthorhombic in a wurtzite superstructure type while Cu₂MnSnS₄ crystallizes in a tetragonal sphalerite superstructure type. Lattice constants and thermal analyses of the solid solution series Cu₂MnGe_xSn_1−xS₄ are presented. A two-phase region is found from Cu₂MnGe_0.3Sn_0.7S₄ to Cu₂MnGe_0.5Sn_0.5S₄. The cell volume of the mixed crystals increases with increasing Sn content. The melting points increase smoothly with increasing Ge content to x=0.5 and then steeply for higher Ge contents. The single crystal X-ray structure analysis of Cu₂MnGe_0.55Sn_0.45S₄ is presented. The refinement converges to R=0.0270 and wR₂=0.0586, Z is 2. The volumes of the tetrahedra [MS₄] (M=Cu, Mn, Ge, Sn) are calculated. From these volumes the differences in size of the tetrahedra are derived and compared with the corresponding differences in the end members of the solid solution series. It turns out that the resulting structure type in these materials depends on the volume differences of the constituting tetrahedra [MS₄].     

Atomic ordering in the doped rare earth cobaltates Ln0.33Sr0.67CoO3−δ (Ln=Y, Ho and Dy)

The perovskite-based rare earth cobaltates (Ln_0.33Sr_0.67CoO_3−δ) (Ln=Y³⁺, Ho³⁺ and Dy³⁺) have been synthesized at 1100°C under 1 atm oxygen. A thermogravimetric study has determined the overall oxygen content in each case while a combined electron diffraction (ED) and synchrotron X-ray diffraction study has revealed the presence of a complex, previously unreported, perovskite-related superstructure phase. ED gave a resultant C1c1 but most probably Cmcm (, , ) perovskite-related superstructure, describable as a modulated I4/mmm intermediate parent structure. Synchrotron X-ray data has been used to refine the intermediate parent structures of all three compounds. Coupled Ln/Sr and O/vacancy ordering and associated structural relaxation is shown to be responsible for the observed superstructure.     

Paracrystalline order in polymers

Summary A brief review of one and three dimensional models of paracrystalline superstructures in polymers, as used for analysing the small angle scattering, is given.

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Zusammenfassung Es wird ein knapper überblick über die bei der Analyse der Kleinwinkelstreuung von Polymeren verwendeten einund dreidimensionalen Modelle der Überstruktur gegeben.

     

Synthesis, crystal structures and ionic conductivities of Bi14P4O31 and Bi50V4O85. Two members of the series Bi18−4mM4mO27+4m (M=P, V) related to the fluorite-type structure

The two hitherto unknown compounds Bi₁₄P₄O₃₁ and Bi₅₀V₄O₈₅ were prepared by the direct solid-state reaction of Bi₂O₃ and (NH₄)H₂PO₄ or V₂O₅, respectively. Bi₁₄P₄O₃₁ crystallizes in a C-centred monoclinic symmetry (C2/c space group) with the unit-cell parameters: , , and β=93.63(1)° (Z=16). The symmetry of Bi₅₀V₄O₈₅ is also monoclinic (I2/m space group) with lattice parameters of , , and β=90.14(1)° (Z=2). Both structures correspond to a fluorite-type superstructure where the Bi and P or V atoms are ordered in the framework. An idealized structural model is proposed where the structures result of the stacking of mixed atomic layers of composition [Bi₁₄M₄O₃₁] and [Bi₁₈O₂₇] respectively. This new family can be formulated Bi_18−4mM_4mO_27+4m with M=P, V and where the parameter m (0?m?1) represents the ratio of the number of [Bi₁₄M₄O₃₁] layers to the total number of layers in the sequence. Bi₁₄P₄O₃₁ corresponds to m=1 when Bi₅₀V₈O₈₅ corresponds to m=1/3. In this last case, the structural sequence is simply one [Bi₁₄V₄O₃₁] layer to two [Bi₁₈O₂₇] layers. As predicted by the proposed structural building principle, Bi₁₄P₄O₃₁ is not a good ionic conductor. The conductivity at 650 °C is 4 orders of magnitude lower from those found in Bi₄₆M₈O₈₉ (M=P, V) (m=2/3) and Bi₅₀V₄O₈₅ (m=1/3).     

The phase diagram and tetragonal superstructures of the rare earth cobaltate phases Ln1−xSrxCoO3-δ (Ln=La, Pr, Nd, Sm, Gd, Y, Ho, Dy, Er, Tm and Yb)

Single phase perovskite-based rare earth cobaltates (Ln_1−xSr_xCoO_3−δ) (Ln=La³⁺, Pr³⁺, Nd³⁺, Sm³⁺, Gd³⁺, Dy³⁺, Y³⁺, Ho³⁺, Er³⁺, Tm³⁺ and Yb³⁺; 0.67?x?0.9) have been synthesized at 1100°C under 1 atmosphere of oxygen. X-ray diffraction of phases containing the larger rare earth ions La³⁺, Pr³⁺ and Nd³⁺ reveals simple cubic structures; however electron diffraction shows orientational twinning of a local, tetragonal (I4/mmm; a_p×a_p×2a_p) superstructure phase. Orientational twinning is also present for Ln_1−xSr_xCoO_3−δ compounds containing rare earth ions smaller than Nd³⁺. These compounds show a modulated intermediate parent with a tetragonal superstructure (I4/mmm; 2a_p×2a_p×4a_p). Thermogravimetric measurements have determined the overall oxygen content, and these phases show mixed valence (3⁺/4⁺) cobalt oxidation states with up to 50% Co(IV). X-ray diffraction data and Rietveld techniques have been used to refine the structures of each of these tetragonal superstructure phases (Ln=Sm³⁺-Yb³⁺). Coupled Ln/Sr and oxygen/vacancy ordering and associated structural relaxation are shown to be responsible for the observed superstructure.     

基于改进的Monte Carlo方法及其应用

建立了一个基于网格由狼羊草组成的生态系统模型，模型中对捕食者(狼)及被捕食者(羊)给予了相应的属性定义，把草界定为可再生资源，通过引入“超结构”的规则，解决了采用Monte Carlo。方法模拟时网格状态不能同步更新的问题。通过模拟，得到模型的三种典型结果：即捕食者灭绝，捕食者被捕食者都灭绝以及捕食者被捕食者共存，给出了三种结果出现的几率分布，而且只要捕食者的初始密度不太大，生态系统很容易达到共存状态，生态系统对应的网格规模越大，生态系统越容易达到共存。     

球状多孔Pd纳米粒子超结构的合成及其对甲酸的电催化氧化

在丙酮／水混合溶剂中,以氯代十六烷基吡啶为结构导向剂,水合肼还原PdCl42-,制得了直径范围在30～50nm之间的球状多孔Pd纳米粒子超结构．实验表明,氯代十六烷基吡啶对球状多孔Pd纳米粒子超结构的形成起着重要的作用,不加该表面活性剂时,得到的是实心Pd纳米粒子;而丙酮主要影响表面活性剂胶束的尺寸．此外,本文还研究了球状多孔Pd纳米粒子超结构对甲酸氧化的电催化活性,在0．5mol／L H2SO4＋0．5mol／L HCOOH溶液中的循环伏安结果表明,球状多孔Pd纳米粒子超结构修饰电极在酸性溶液中电催化氧化甲酸的峰电流约为180mA／mg,明显优于实心Pd纳米粒子修饰电极（峰电流为120mA／mg）,且表现出较高的稳定性．