Study of the island morphology at the early stages of Fe/Mo(110) MBE growth

We present theoretical study of morphology of Fe islands grown at Mo(110) surface in submonolayer MBE mode. We utilize atomistic SOS model with bond counting, and interactions of Fe adatom up to third nearest neighbors. We performed KMC simulations for different values of adatom interactions and varying temperatures. We have found that, while for the low temperature islands are fat fractals, for the temperature 500 K islands have faceted rhombic-like shape. For the higher temperature, islands acquire a rounded shape. In order to evaluate qualitatively morphological changes, we measured average aspect ratio of islands. We calculated dependence of the average aspect ratio on the temperature, and on the strength of interactions of an adatom with neighbors.      

Elements of Prescribed Order,Prescribed Traces and Systems of Rational Functions Over Finite Fields

Let k 1 and be a system of rational functions forming a strongly linearly independent set over a finite field . Let be arbitrarily prescribed elements. We prove that for all sufficiently large extensions , there is an element of prescribed order such that is the relative trace map from onto We give some applications to BCH codes, finite field arithmetic and ordered orthogonal arrays. We also solve a question of Helleseth et~al. (Hypercubic 4 and 5-designs from Double-Error-Correcting codes, Des. Codes. Cryptgr. 28(2003). pp. 265–282) completely.classification 11T30, 11G20, 05B15     

有序介孔氧化硅薄膜制备及其组装化学

本文综述了近年来利用有机模板法合成有序介孔二氧化硅薄膜的研究进展，重点阐述了两相界面外延生长和蒸发诱导自组装两种制备方法及其合成机理。此外，讨论了有序介孔二氧化硅薄膜的组装化学，包括金属元素掺杂，纳米粒子在介孔薄膜中的组装，以及有机物/二氧化硅纳米复合薄膜的制备，并对介孔二氧化硅薄膜未来的发展趋势做了展望。     

光调控分子有序聚集体及其功能化研究进展

双亲分子在溶液中可以缔合形成胶束、囊泡、液晶、乳液等有序分子聚集体。在分子中引入功能性的基团,通过改变分子的结构、浓度或引入外部刺激,可以对有序分子聚集体的类型和性能进行调控。光作为一种绿色可控的清洁能源,是一种理想的外部刺激信号。在双亲分子中引入感光基团,可以通过光照调节有序聚集体的组装,并进一步实现功能性的调控。本文综述了近年来在光调控分子有序聚集体方面的研究及其在生物、传导、纳米材料制备中的应用。同时,对光调控的功能性有序分子聚集体未来的发展前景进行了展望。     

三维有序大孔Fe_2SiO_4/SiO_2@C锂离子电池负极纳米玻璃陶瓷-碳复合材料制备及电化学性能

以聚苯乙烯(PS)胶晶作为铸模,采用纳米铸造工艺及后续煅烧的方法合成了三维有序大孔Fe_2SiO_4/SiO_2@C纳米玻璃陶瓷锂离子电池负极材料。溶胶-凝胶工艺产生的凝胶在650℃氩气氛炉中煅烧后,Fe_2SiO_4纳米晶体从含铁元素的SiO_2基玻璃中结晶析出,形成由Fe_2SiO_4纳米晶体、铁离子(Fe3+)修饰的玻璃态SiO_2和非晶碳组成的三维有序大孔纳米玻璃陶瓷。在50 m A·g~(-1)电流密度下进行充放电时,其放电容量可达450 m Ah·g~(-1)以上,电流密度增加到250 m A·g~(-1)时可逆放电容量仍旧稳定地保持在260 m Ah·g~(-1),而具有同样有序大孔结构和含碳量的非晶态SiO_2@C材料的放电比容量在50 m A·g~(-1)电流密度时仅为15 m Ah·g~(-1)。这些结果表明,Fe_2SiO_4纳米晶体及Fe~(3+)有助于SiO_2基玻璃陶瓷实现可逆储锂过程。     

La、Ce、Yb掺杂对LiNi0.5Mn1.5O4高电压正极材料性能的影响

采用低温燃烧法制备出不同稀土元素掺杂的高电压镍锰酸锂(LiNi_(0.5)Mn_(1.5)O_4)正极材料,探究了不同掺杂比例(物质的量分数0.5%、1%、2%)和不同掺杂稀土元素(La、Ce、Yb)对样品性能的影响,并通过X射线衍射、拉曼光谱、电子顺磁共振和恒电流间歇滴定等技术探究了其影响机理。从X射线衍射图可以看出,稀土掺杂可以抑制Li_xNi_(1-x)O杂质相的产生;电感耦合等离子谱结果表明,掺杂进入的稀土元素与设计比例基本相符;从拉曼光谱图可以看出,稀土元素可以使样品的有序相增多,其中Ce掺杂样品的有序相最多;结合电子顺磁共振波谱氧空位测试,发现Ce掺杂诱导了样品中有序相比例增加,从而使样品的稳定性提高;经恒电流间歇滴定技术测试发现,Ce掺杂镍锰酸锂样品的扩散系数比未掺杂样品高了约15倍;在不同掺杂比例上,1%掺杂量时样品性能最佳。在3种最佳掺杂量的稀土元素样品中,Ce掺杂的样品性能最优,首次放电比容量可以达到133.3mAh·g~(-1),比未掺杂样品放电比容量高且首次效率提高了 18%,在1C下循环200次后,容量保持率为102%,比未掺杂样品提高了 8%。     

Carbon nanotube and carbon nanorod-filled polyacrylonitrile electrospun stationary phase for ultrathin layer chromatography

The application of carbon nanotube or nanorod/polyacrylonitrile (PAN) composite electrospun nanofibrous stationary phase for ultrathin layer chromatography (UTLC) is described herein. Multi-walled carbon nanotubes (MWCNTs) and edge-plane carbon (EPC) nanorods were prepared and electrospun with the PAN polymer solution to form composite nanofibers for use as a UTLC stationary phase. The analysis of laser dyes demonstrated the feasibility of utilizing carbon nanoparticle-filled electrospun nanofibers as a UTLC stationary phase. The contribution of MWCNT or EPC in changing selectivity of the stationary phase was studied by comparing the chromatographic behavior among MWCNT–PAN plates, EPC–PAN plates and pure PAN plates. Carbon nanoparticles in the stationary phase were able to establish strong π–π interactions with aromatic analytes. The separation of five polycyclic aromatic hydrocarbons (PAHs) demonstrated enhanced chromatographic performance of MWCNT-filled stationary phase by displaying substantially improved resolution and separation efficiency. Band broadening of the spots for MWCNT or EPC-filled UTLC stationary phases was also investigated and compared with that for pure PAN stationary phases. A 50% improvement in band dispersion was noted using the MWCNT based composite nanofibrous UTLC plates.     

高比表面积有序介孔Ni/SiC催化CH4-CO2重整反应

采用纳米浇铸法制备了高比表面积（345 m²/g）且孔径均一的有序介孔SiC材料（SiC-OM），以商用SiC（49 m²/g，SiC-C）材料为参比载体。采用等体积浸渍法分别制备了Ni/SiC-OM和Ni/SiC-C，并考察其在CH₄-CO₂重整反应中的催化性能。利用ICP、BET、XRD、H₂-TPR、XPS、HRTEM、TG和Raman等手段对反应前后的两种催化剂进行表征。结果表明，在700℃、1.013×10⁵ Pa和12 L/（h·g）的重整条件下，Ni/SiC-OM的平均积炭速率比Ni/SiC-C降低了一个数量级，这主要归因于强金属-载体相互作用和有序介孔骨架的"限域效应"作用。     

聚苯乙烯/蒙脱土纳米复合材料中的剪切诱导有序结构(Ⅰ)——广角X射线衍射与透射电镜研究

聚合物/层状硅酸盐(PLS)纳米复合材料是近10余年来迅速发展起来的的交叉学科.由于其具有常规复合材料所没有的结构、形态以及较常规聚合物基复合材料更优异的性能等而引起人们的广泛关注[1].以往文献主要报道PLS纳米复合材料的制备与性能表征,如尼龙-6/蒙脱土[2]、PET/蒙脱土[3]和硅橡胶/蒙脱土[4]等.对于熔融加工过程中粘土片层及高分子的取向和结构研究很少.Kojima等[5]发现并研究了尼龙-6/蒙脱土纳米复合材料中的熔融剪切诱导取向结构,其X射线衍射与透射电镜(TEM)结果均表明,粘土片层沿熔体流动方向平行取向,但片层间距不等,因此为一平行取向但无序的结构.对于PLS纳米复合材料中的剪切诱导有序结构尚未见报道.     

Preparation and characterization of three-dimensionally ordered macroporous yttria-stabilized zirconia by aqueous organic gel route

Three-dimensionally ordered macroporous (3-DOM) yttria-stabilized zirconia (YSZ) was prepared by aqueous organic gel method through the interstitial spaces between polystyrene spheres assembled on glass substrates. The morphologies and pore size of the porous YSZ were characterized by scanning electron microscope (SEM) and nitrogen adsorption. The thermal behavior, the phase and chemical composition of PS/YSZ composite were investigated by Fourier transform infrared spectroscopy (FT-IR), X-ray diffraction (XRD) and X-ray photoelectron spectroscopy (XPS). The results show that porous YSZ has been formed with the pores arranged in an ordered close-packed three-dimensional structure. Ni/YSZ cermet was also prepared by immersing the 3-DOM YSZ into the solution of nickel nitrate and urea. The electrical conductivity of Ni/YSZ was about 400 S cm⁻¹ between 600 and 800 °C.