一种改进的用于Adams预估-校正算法的步长控制方法

1 引 言 对于一阶常微分方程 y'=f(t,y).(1) 的数值解法,目前常用的主要有两类方法:单步法和线性多步法(Linear Multistep Methods,LMM).     

用单调性证明数列的连续项积型不等式

对数列连续项积型不等式，文[1]给出了用其成立的一个充分条件证明的方法．笔者探究发现，用单调性证明某些此类不等式更简便．     

Preparation of high performance thin-film polarizers

<正>The optical performance of thin film polarizers is highly sensitive to the layer thicknesses of thin film.The thicknesses of the sensitive layers are optimized in order to gain broader polarizing zone in such case when the total layer thickness does not increase.An automatic layer thickness control system is established,and errors caused by different monitoring methods are analyzed.With this thickness control system,thin-film polarizers with T_p higher than 98%and T_p/T_s higher than 200:1(T_p and T_s are transmissions for p- and s-polarizations,respectively) with the bandwidth of 11 nm are prepared.Using the system allows for optimum repeatability of three successive runs.     

臭氧层的化学破坏及其对策

臭氧层的化学破坏是人类的重大环境问题。本文对臭氧层的形成，作用，臭氧层破坏的后果，破坏臭氧层的物质及作用机制和保护臭氧层的对策作了探讨。     

一种邻近性的计算方法

邻近律是Gestalt定律的基本定律之一，然而迄今为止，如何在图像处理中计算元素之间的邻近性程度还没有具体方法提出．以点元素作为抽象载体提出了一种邻近性的计算方法，该方法借鉴基于最小支撑树（MST）的聚类思想，引入三角剖分和Prim算法计算元素之间的MST邻近性测度和加权MST邻近性测度用于度量元素之间的邻近性．实验结...     

微量Co修饰的碳载超细Pt纳米粒子的制备及其在燃料电池氧还原催化中的应用

质子交换膜燃料电池(PEMFC)具有清洁、高效等优点,是一种理想的汽车动力电源.然而,由于其阴极氧还原反应(ORR)速率缓慢,需要使用大量的Pt基催化剂,导致燃料电池成本居高不下,严重制约了PEMFC的商业化发展.将Pt与过渡金属Fe, Co, Ni等形成合金,对表面Pt原子的几何结构和电子结构进行调变,可以有效提高催化剂的活性,实现Pt用量和燃料电池成本的降低.但是目前合金催化剂多采用溶剂热、浸渍-高温退火等制备方法,使用有毒有害试剂和难清洗的表面活性剂,且过程复杂、能耗高,不利于大规模化生产.此外,合金中过渡金属占比高,在燃料电池工况下,大量过渡金属溶解,加速了膜的降解,导致实际PEMFC性能的降低.对此,我们探索了一种简便有效的方法制备高活性、高稳定性的碳载Pt-Co催化剂.在没有添加表面活性剂的情况下,采用硼氢化钠辅助乙二醇还原法合成了具有超小尺寸和均匀分布的Pt-Co纳米颗粒,后续酸刻蚀处理去除不稳定的Co原子,重组双金属纳米颗粒的表面结构形成富Pt壳层,进一步提高了催化剂的活性和稳定性.通过电感耦合等离子体、X射线粉末衍射、透射电子显微镜、高分辨透射电子显微镜、高角环形暗场-扫描透射-元素分布及光电子能谱等物理表征证实了微量Co改性的碳载超细铂合金纳米颗粒的组成和结构.进一步对催化剂进行旋转圆盘电极和单电池测试,结果表明, Pt_(36)Co/C具有明显高于商业化Pt/C的有效电化学活性面积和电池性能.此外,加速衰减测试和衰减前后的电镜图片表明, Pt_(36)Co/C催化剂的稳定性相较于Pt/C亦有所增强.分析Pt-Co/C催化性能提高的原因,主要归于以下三点:(1)催化剂纳米颗粒在载体上分布均匀,且具有超小的粒径尺寸,提供了大量的三相反应界面位点;(2)双金属配体和电子效应的协同作用,降低了氧化物质在催化表面的吸附能力,加速了ORR的电催化动力学;(3)酸蚀刻导致的不稳定Co的溶解及催化剂表面结构的重排,形成了富Pt壳层结构,有利于提高催化剂的稳定性.这种简单有效的合金制备方法可以在电催化领域推广使用.     

微波辅助制备均分散PbS纳米棒

在十二烷基苯磺酸钠存在下,以0．5℃．h^-1的速度均匀降温48h,微波辅助成核合成均分散PbS纳米棒。实验结果表明微波辐照促进一次成核,抑制二次成核,是形成PbS纳米棒的关键。PbS纳米棒的结构经X-射线粉末衍射,透射电子显微镜和荧光光谱表征。     

Graded index broadband antireflection coating prepared by glancing angle deposition for a high-power laser system

This paper reports that SiO₂ is selected to fabricate broadband antireflection (AR) coatings on fused silica substrate by using glancing angle deposition and physical vapour deposition. Through accurate control of the graded index of the SiO₂ layer, transmittance of the graded broadband AR coating can achieve an average value of 98% across a spectral range of 300--1850~nm. Moreover, a laser-induced damage threshold measurement of the fabricated AR coating is performed by using a one-on-one protocol according to ISO11254-1, resulting in an average damage threshold of 17.2~J/cm$^{2}$.     

土壤中多环芳烃和酞酸酯类有机污染物气相色谱-质谱测定方法中的质量控制与质量保证

建立了气相色谱-质谱(GC-MS)测定土壤中多环芳烃(PAHs)和酞酸酯类(PAEs)有机污染物的方法。样品经加速溶剂萃取和超声萃取处理后,通过固相萃取或凝胶渗透色谱法进行净化,在选择离子监测模式下进行定量。通过全程序空白、空白加标回收、清洁土壤基质加标回收及有证标准参考物质比对等方式,对所建立的方法进行严格的质量控制和保证。16种PAHs和7种PAEs的方法检出限分别为0.13～2.2 μg/kg和0.19～0.52 μg/kg,平均加标回收率分别为41.5%～116.9%和90.7%~107.1%。本研究所建立的土壤中PAHs和PAEs的GC-MS快速分析方法及其质量控制措施可以为全国性土壤污染状况调查数据的科学性和准确性提供技术保障。     

Orientation dependence of structural transition in fcc Al driven under uniaxial compression by atomistic simulations

By molecular dynamics simulations employing an embedded atom method potential,we have investigated structural transformations in single crystal Al caused by uniaxial strain loading along the [001],[011] and [111] directions. We find that the structural transition is strongly dependent on the crystal orientations. The entire structure phase transition only occurs when loading along the [001] direction,and the increased amplitude of temperature for [001] loading is evidently lower than that for other orientations. The morphology evolutions of the structural transition for [011] and [111] loadings are analysed in detail. The results indicate that only 20% of atoms transit to the hcp phase for [011] and [111] loadings,and the appearance of the hcp phase is due to the partial dislocation moving forward on {111} fcc family. For [011] loading,the hcp phase grows to form laminar morphology in four planes,which belong to the {111} fcc family; while for [111] loading,the hcp phase grows into a laminar structure in three planes,which belong to the {111} fcc family except for the (111) plane. In addition,the phase transition is evaluated by using the radial distribution functions.