(La_xNd_y)_(0.90)Mg_(0.10)Ni_(3.09)Mn_(0.12)Co_(0.60)Al_(0.13)贮氢合金自放电性能研究

为了提高La-Mg-Ni基贮氢合金的荷电保持率,本文研究了La/Nd比的变化对La-Mg-Ni基贮氢合金自放电性能的影响。随着Nd替代La量的增加,(LaxNdy)0.9Mg0.10Ni3.09Mn0.12Co0.60Al0.13(x/y=5,4,3,2,1)合金的荷电保持率先增大后减小,当x/y=4时,其荷电保持率达到最大值80.8%(318 K)。合金电极贮存后,FESEM-EDS和XRD分析表明,合金颗粒表面形成了Mg(OH)2和Nd(OH)3。P-C-T曲线和Tafel极化测试表明,随着Nd含量的增加,金属氢化物的稳定性呈现先增加后降低和腐蚀电流先减小后增大的规律。     

(Fe_(0.86)Zr_(0.033)Nb_(0.033)B_(0.068)Cu_(0.01))_x(Al_2O_3)_(1-x)颗粒膜的霍耳效应

用磁控溅射方法制备了系列 (Fe0 .86 Zr0 .0 33Nb0 .0 33B0 .0 6 8Cu0 .0 1 ) x(Al2 O3) 1 -x颗粒膜样品 ,体积百分比x从 0 .3 3～ 0 .63 ,样品厚度约为10 0nm。室温下在Fe0 .86 Zr0 .0 33Nb0 .0 33B0 .0 6 8Cu0 .0 1 体积百分比x =0 .43时得到 17.5 μΩ·cm的最大饱和霍耳电阻率 ,比纯铁磁金属提高了 3～ 4个量级。对其磁性和微结构进行了研究 ,样品霍耳电阻率随外场的变化曲线 ρxy～H与磁场平行于膜面时的磁化曲线M～H有相似性 ,说明霍尔电阻率 ρxy与磁化强度M相关。样品电阻率 ρxx随金属体积百分比x的减小而增加 ,在x =0 .43附近发生突变 ,从金属导电变为绝缘体。根据微结构和输运性质对可能的机制进行了探讨     

La_(1.1)Fe_(11.4)Si_(1.55)Ge_(0.05)合金的磁热效应

使用电弧熔炼法制备了La1.1Fe11.4Si1.55Ge0.05合金。研究了用少量的Ge替代Si后,La1.1Fe11.4Si1.55Ge0.05合金的磁性和磁热效应。粉末X射线衍射结果表明:在1273K真空退火处理10d后,合金La1.1Fe11.4Si1.55Ge0.05主相为NaZn13型立方结构,存在微量的α-Fe相。热磁曲线M-T与Arrott曲线表明:在居里温度Tc=205K处发生由铁磁性(TTc)转变为顺磁性(TTc)的二级磁相变。在磁场变化0～1.5T下,根据等温磁化曲线通过Maxwell关系式计算得出最大磁熵变-ΔSmmax=9J.kg-.1K-1。Ge替代Si后该合金在其居里温度Tc处-ΔSm-T曲线半高宽增大,使合金的相对制冷能力RCP(S)有所提高。     

Indentation creep behaviors of Mg61Cu28Gd11 and （Mg61Cu28Gd11）99.5Sb0.5 bulk metallic glasses at room temperature

The room temperature creep behaviors of Mg61Cu28Gd11 and(Mg61Cu28Gd11)99.5Sb0.5 bulk metallic glasses(BMGs) were revealed by means of nanoindentation technique.The creep mechanism was explored by characterization of creep rate sensitivity,creep compliance and retardation spectra.The results showed that the experimental creep curves could be well described by a generalized Kelvin model.The low creep rate sensitivity of both Mg-based BMGs indicated that their room temperature creep was dominated by localized shear flow.In addition,the(Mg61Cu28Gd11)99.5Sb0.5 glassy alloy exhibited lower creep rate sensitivity,creep compliance and milder retardation peak,indicating its higher creep-resistance and less relaxed state.Furthermore,the creep retardation spectrum consisted of two relatively separated peaks with the well defined characteristic relaxation times.     

Structure and Magnetic Properties of Y(Fe_(1-x) Co_x)_ (11.3) Nb_(0.7)

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Kinetics of Hydrogen Absorption in MmNi_（3．55）Co_（0．75）Mn_（0．4）Al_（0．3） Alloy

ＫｉｎｅｔｉｃｓｏｆＨｙｄｒｏｇｅｎＡｂｓｏｒｐｔｉｏｎｉｎＭｍＮｉ_（３．５５）Ｃｏ_（０．７５）Ｍｎ_（０．４）Ａｌ_（０．３）ＡｌｌｏｙＬｉｎＱｉｎ（林勤），ＹｕＺｈｅｎｔａｏ（于振涛），ＹｅＷｅｎ（叶文）（ＵｎｉｖｅｒｓｉｔｙｏｆＳｃｉｅｎｃｅａ...     

快速热压制备(AgSbTe_2)_x(Pb_(0.5)Sn_(0.5)Te)_(1-x)半导体材料及热电性能研究

为了进一步提高PbTe系列合金的热电性能和降低生产成本,采用溶剂热反应合成平均粒度为500 nm的PbTe粉末,以所合成的PbTe粉末为主要原料通过封管熔炼法制备(AgSbTe2)x(Pb0.5SnvTe) 1-x(x=0,0.05,0.1,0.15,0.2)系合金.所得合金锭经过高能球磨制成微米级的超细合金粉,再通过快速热压烧结制备测试用的多晶试样,所有试样的相对密度均达到90%以上.通过XRD和SEM等手段分析材料的物相组成和微观结构,研究x的变化对于该体系材料热电性能(电阻率、Seebeck系数、热导率和ZT值)的影响.研究表明,当X取值为0.1时该体系材料的热电性能得到最优化,在575 K时取得最人的ZT值为1.093.     

Magnetocaloric effect and magnetic properties of La_（0.9）Ce_（0.1）（Fe_（0.99）Mn_（0.01））_（11.6）Si_（1.4）H_（1.6） compound

Magnetocaloric effect and magnetic properties of La0.9Ce0.1(Fe0.99Mn0.01)11.6Si1.4 and its hydride La0.9Ce0.1(Fe0.99Mn0.01)11.6Si1.4H1.6 were investigated. The Curie temperature of La0.9Ce0.1(Fe0.99Mn0.01)11.6Si1.4 was increased by hydrogen absorption. XRD patterns showed that the structure of La0.9Ce0.1(Fe0.99Mn0.01)11.6Si1.4H1.6 remained NaZn13-type. The Curie temperature (TC) of the sample was increased from 174 K to 331 K. The homogeneity of the hydrogen absorption for La0.9Ce0.1(Fe0.99Mn0.01)11.6Si1.4H1.6 was proven very well by the random measurement of DSC. The magnetic entropy △SM of La0.9Ce0.1(Fe0.99Mn0.01)11.6Si1.4H1.6 had peak at 326 K. The peak value of-△SM-was 12.3 and 7.8 J/(kg.K) under magnetic field change of 0-2 T and 0-1 T,respectively,which was comparable with Gd5Si2Ge2. The negative slope and inflection point of the Arrott curve indicated that the first-order magnetic transition of La0.9Ce0.1(Fe0.99Mn0.01)11.6Si1.4 was reserved after hydrogen absorption.     

酒石酸-硝酸盐低热固相反应制备Ni_(0.18)Cu_(0.2)Zn_(0.62)O(Fe_2O_3)_(0.98)铁氧体

以酒石酸和金属硝酸盐为原料,采用低热固相反应方法合成了Ni0.18Cu0.2Zn0.62O(Fe2O3)0.98尖晶石型铁氧体,并应用FT-IR,DSC-TG,XRD,TEM以及SEM等技术对低热固相反应过程和样品进行了研究和表征。FT-IR研究表明,酒石酸和金属硝酸盐在研磨30min后发生了低热固相反应,生成金属酒石酸盐前驱体。FT-IR和XRD分析表明,前驱体经不同温度焙烧后得到单一尖晶石相的NiCuZn铁氧体粉。依据谢乐公式计算和TEM表征,证明干凝胶在350℃分解1h后的粒径约为20～30nm,将此粉体在750℃下焙烧2h后,粒径增大到100～150nm。铁氧体于900℃烧结为陶瓷体后,晶粒约为2～4μm,烧结致密。随着烧结温度由850℃提高到900℃,NiCuZn铁氧体的矫顽力Hc有所下降,但饱和磁化强度Ms有所升高。磁谱测量表明,900℃烧结样品的磁导率为170,截止频率为32MHz,样品的磁性主要来源于畴壁位移的贡献。     

Stability of triple-helical poly(dT)-poly(dA)-poly(dT) DNA with counterions

Structural conformation of triple-helical poly(dT)-poly(dA)-poly(dT) has been a very controversial issue recently. Earlier investigations, based on fiber diffraction data and molecular modeling, indicated an A-form conformation with C'3-endo sugar pucker. On the other hand, Raman, solution infrared spectral, and NMR studies show a B-form structure with C'2-endo sugars. In accordance with these experimental results, a theoretical model with B-form, C'2-endo sugars was proposed in 1993. In the present work we investigate the dynamics and stability of the two conformations within the effective local field approach applied to the normal mode calculations for the system. The presence of counterions was explicitly taken into account. Stable equilibrium positions for the counterions were calculated by analyzing the normal mode dynamics and free energy of the system. The breathing modes of the triple helix are shifted to higher frequencies over those of the double helix by 4-16 cm-1. The characteristic marker band for the B conformation at 835 cm-1 is split up into two marker bands at 830 and 835 cm-1. A detailed comparison of the normal modes and the free energies indicates that the B-form structure, with C'2-endo sugar pucker, is more stable than the A-form structure. The normal modes and the corresponding dipole moments are found to be in close agreement with recent spectroscopic findings.     

La_(0.67)Sr_(0.33)MnO_3/La_(0.75)MnO_(0.67)Sr_(0.33)MnO_3庞磁电阻三层膜的制备及结构形貌和性能

用磁控溅射法在 (0 0 1)取向的LaAlO3单晶基片上制备了La0 .6 7Sr0 .33MnO3/La0 .75MnO3/La0 .6 7Sr0 .33MnO3外延三层膜。结果表明 ,与La0 .6 7Sr0 .33MnO3单层膜相比较 ,外延三层膜的X射线衍射图上出现 3级衍射峰 ,每级衍射峰由 3个峰组成 :其中强度最高的衍射峰代表衬底的衍射 ;次强的代表上下两层La0 .6 7Sr0 .33MnO3膜 ;最弱的代表中间La0 .75MnO3层。三层膜的二维原子力表面形貌为均匀的小颗粒状 ,表明其三维形貌为外延岛状柱状晶。这种三层膜的巨磁电阻效应与中间层La0 .75MnO3的厚度有关 ,当中间层厚度为 70nm时 ,其最大磁电阻值可达到 3 2 % ,这个结果优于La0 .6 7Sr0 .33MnO3单层膜的巨磁电阻效应。其可能的原因是电子在界面上的散射、层间的交互作用 ,以及点阵错配导致的内应力的综合结果。     

Osteodysplasty (Melnick-Needles syndrome) (author's transl)

Authors report a new case of osteodisplasty (Melnick-Needles syndrome) and describe radiological findings that are typical of this entity: bony sclerosis of base structures, abnormal dental alignment, sclerosis and irregularity of clavicles and ribs, described as "band-like" deformity, cortical irregularity of tubular bones with metaphyseal flaring and diaphyseal bowing. Flat bones are broadened, particularly iliac crest and vertebral bones. Facial features described by the majority of authors in this entity are present in our patient in an incomplete form: craniofacial disproportion, micrognatia, depressed temples, exophthalmus (not in our patient) and broadened forehead. The paper is intended to gather clinical data of already reported cases in order to facilitate clinical research in the future from the immunological, genetical and biochemical points of view. Our patient has the same clinical history as the patient studied in the original paper. Dr. Melnick was kind enough to send us clinical data and autopsy findings.     

Crystal Structure of Ni_(50)Mn_(29)Ga_(21)Tb_(1.2) Magnetic Shape Memory Alloy at Room Temperature

Crystal Structure of Ni_(50)Mn_(29)Ga_(21)Tb_(1.2) Magnetic Shape Memory Alloy at Room Temperature     

激光处理制备La_(0.6)Ba_(0.4)Co_(0.2)Fe_(0.8)O_3钙钛矿催化剂

通过柠檬酸络合树脂法合成了钙钛矿催化剂La0.6Ba0.4Co0.2Fe0.8O3前驱体,然后分别对前驱体以不同功率和扫描速度的激光扫描及高温焙烧进行处理。用XRD、XPS方法测定了催化剂的结构并测定了催化剂的甲烷燃烧活性。结果表明,适当激光条件下制备的催化剂活性明显高于高温焙烧的催化剂。激光制备催化剂高活性的原因可归因于,激光处理的特点使催化剂形成较小的晶粒度、存在的夹杂相造成晶格缺陷。