UFeGa5单晶生长及晶体结构研究

采用镓自助熔剂的方法生长出了UFeGa5单晶,采用X射线衍射技术和Rietveld方法对UFeGa5晶体结构进行了研究。结果表明:生长出的UFeGa5单晶体结构完整,结晶性好。UFeGa5具有HoCoGa5型四方结构,空间群为P4/mmm(No.123),其晶格常数为a=0.42533(2)nm,c=0.67298(3)nm,并得到了透射电镜(TEM)实验验证。     

高温淬火Co_(72.7)C_(11.8)Si_(15.5)磁性合金的结构和相转变

用X射线衍射、透射电子显微镜、场致发射扫描电镜和电子探针研究了Co72 .7C11.8Si15.5合金在 10 0 0℃均匀化退火 7d后 ,水淬至室温的相变和相结构。结果表明 :合金由两个相组成 ,一个是具有密排六方 (hcp)结构的基体Co固溶体 ,其晶格常数a =0 .2 5 0 5nm ,c=0 .40 73nm ;另一个是具有六方 (hex)结构的第二相石墨 ,其晶格常数a =0 .2 46 5nm ,c =0 .6 711nm。X射线衍射没有探测到高温fcc Co相的 (2 0 0 )衍射峰 ,表明fcc Co相已完全转变为hcp Co相 ,平衡转变温度在 10 0 0℃以上。在Co金属中复合添加C和Si元素可以容易地获得室温稳定的hcp结构。     

爆炸压结Nd-Fe-B永磁体微观结构

利用透射电镜、X射线衍射仪、X射线能谱仪，对爆炸压结Nd-Fe-B永磁合金进行微观组织结构的观察和分析。结果表明：爆炸压结Nd-Fe-B的组织主要由基体Nd2Fe14B相、富O相和富Nd相组成；基体相是硬磁相，四方晶体结构，其晶格常数为a=0．88nm和c=1．22nm；富O相形貌呈三角状或层状，分布在3个晶粒交隅处和两个晶粒交界处，其晶体结构均为面心立方（fcc），点阵常数a=0.559nm；富Nd相呈不同块状形貌，镶嵌存基体内或晶界上，其晶体结构为密排六方（hcp），晶格常数a=0．395nm和c=0.628nm：在富O相中O，Nd和Fe的含量（原子分数，下同）分别为45％～60％，20％～40％和10％～12％，块状富Nd相中则为80％～85％Nd和10％～l5％O，同时还发现晶界相中分布着少量的位错。     

金诺芬的晶体结构研究

用X射线粉末衍射方法 (XRD)对 3种不同熔点的金诺芬 (C2 0 H34AuO9PS)的晶体结构进行研究。结果表明 ,熔点为 1 1 2～ 1 1 4℃的金诺芬属于单斜晶系 ,晶胞参数是a =1 0 30 6nm ,b =0 82 30nm ,c =1 61 62nm ,β =1 0 5 31 6° ;熔点为 1 1 8～ 1 2 0℃的金诺芬属于六方晶系 ,晶胞参数是a =1 462 4 ( 4 )nm ,c =1 1 367( 3)nm ,β =1 2 0° ;熔点为 1 1 4～ 1 1 8℃的金诺芬是单斜晶系和六方晶系晶体组成的混合物。     

抗癌新药JM216的晶体结构分析

用X射线衍射方法分析了顺式 -二氯 -反式 -二乙酸 -顺式 -氨 ,环己胺合铂(IV)〔PtCl2 (C2 H3O2 ) 2 (C6H1 3N) (NH3〕的晶体结构 ,得出了该晶体的粉末衍射数据 ,结果表明 :它属于单斜晶系 ,晶胞参数a =1 360 1 ( 8)nm ,b =0 82 92 ( 2 )nm ,c =1 4682 ( 6)nm ,β =1 1 0 483( 35)°     

不同形貌Ga2O3纳米材料可控合成工艺研究

通过研究基片种类、加热温度、保温时间、冷却速度及是否加入催化剂等不同工艺参数对低维Ga2O3，纳米材料形貌的影响，确定出合成5种不同形貌β-Ga2O3纳米材料的工艺条件。场发射扫描电镜（FE-SEM）表明5种不同形貌α-Ga2O3纳米材料分别为纳米线、纳米棒、纳米带、纳米环及纳米片。X射线衍射（X-ray）分析结果表明不同形貌纳米材料均为晶格常数日=1．223nm，b=0．304nm，c=0．58nm，a=90°，β=103．7°，γ=90°的单斜晶系β-Ga2O3晶体。     

稀土化合物Tm_2(Co_(1-x)Fe_x)_(17)的结构与磁性研究

采用真空悬浮熔炼法制备了Tm_2(Co_(1-x)Fe_x)_(17)(x=0,0.1,0.2,0.3,0.4)化合物。用X射线衍射仪和振动样品磁强计(VSM)研究了封管退火后化合物的晶体结构和磁性。X射线衍射结果表明,化合物都具有单相Th_2Ni_(17)六方结构,属于P63/mmc空间群;Fe元素对Co元素的替代不改变化合物的晶体结构;晶格常数a、c和晶胞体积V都随着Fe含量的增加而增大。磁性测量结果表明,Tm_2(Co_(1-x)Fe_x)_(17)化合物的饱和磁化强度Ms随Fe含量的增加而增大;化合物的各向异性场H_A先增大后减小,x=0.3时达到最大值4.8 T。合适的Fe元素替代可改善化合物的磁性能。     

Pd-20W合金固溶体的结构分析

对Pd－20W合金进行X射线衍射分析和差热分析，结果表明：Pd－20W合金合金是面心立方固溶体，合金的晶格点阵参数和晶粒大小随着温度的变化而变化，在温度缓慢下降至750℃时出现了超结构转变。这表明在Pd－20W合金中的K状太是一种超晶格结构。     

Ca2KNa（PO4）2结构的大角度XRD测定

通过大角度的粉末X射线衍射测定了正磷酸钠钾钙[(Ca2KNa(PO4)2)]晶体陶瓷的晶格参数，分析化学纯度的碳酸钙，磷酸二氢钾、磷酸二氢钠按照2：1：1的摩尔比混合后于1300摄氏度高温反应4h，得到了组合符合Ca2KNa(PO4)2的正磷酸钠钾钙陶瓷，在10度－130度的2θ扫描角范围内，在室温下进行粉末X射线衍射。测定结果显示，高温合成的Ca2KN2(PO4)2晶体相是α－CaKPO4和α－CaNaPO4晶体的高温固溶体，呈六方晶体结构，晶格参数为：α0＝0．54396nm,C0=0.72976nm，晶胞体积V＝0．187nm^3.     

Gd—Pt—In合金系中的新三元化合物GdPt2In

采用高频熔炼合成单相三元化合物GdPt_2In。通过X-射线衍射分析、电子探针和显微金相等方法,确定该化合物具有类似于GdPt_2Sn的六方结构:a=0.4582nm,c=0.9067nm,c/a=1.979,     

Microstructure and transformation behavior of Ni50Ti45Ta5 shape memory alloy

1　INTRODUCTIONTheNiTishapememoryalloy (SMA )iscur rentlyatopicofnotableinterestinmedicine .Itpro videsauniqueopportunitytomakenovelsurgicalim plantsandinstrumentsforminimallyinvasive ,vascu larandorthopedicsurgery .Recently ,NiTiimplantshavebeendevelopedforcardiovascularandgastroin testinalsurgery[13] .ThehighnickelcontentofNiTi(5 4%bymass)cancauseproblemsinbiocompati bilitybecauseoftoxiceffectsofnickel[4 ] .Moreover ,thelowX rayvisibilityofNiTiSMAhaslimitedsomemedicalapplications …     

Crystal Structure and X-ray Powder Diffraction Data for Rare Earth Compound PrNiSn

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ON THE HIGH Tc SUPERCONDUCITVITY OF Y-Ba-Cu OXIDE

<正> 近一年来,在Ba(Sr)-La-Cu-O体系中,陆续发现了一系列高Tc(30—40K)超导体。最近的报道表明,有关超导材料的研究呈现日新月异的飞速进展。本文报道一种起始转变温度为     

STRUCTURE AND MAGNETIC PROPERTIES OF YFe12-xTix COMPOUNDS

1. IntroductionThe discovery of NdZFe14B compound['1 hAs not only led to the appearance of thethird generation of rare-earth permanellt magnets, but also stimulated many researchersto search for novel iron-rich rarerearth ilitermetallic compounds with permanent magnetproperties. In the last decade, investigation of magnetic and structural properties of therare earth (R) transitional metal (T) intermetallic compounds and their nitrides withThMn12-type structure became one of focal points in …     

Crystal Structures of Dy_2(WO_4)_3 and GdY(WO_4)_3

Two compounds, Dy2(WO4)3 and GdY(WO4)3, were synthesized by using the standard solid state reaction technique. The crystal structure was determined by powder X-ray diffraction and Rietveld refinement method. It is found that both compounds have Eu2(WO4)3-type monoclinic structure, with space group C 2/c, Z = 4. The unit cell parameters of Dy2(WO4)3 are a = 0.75981(1) nm. b = 1.13220( 1) nm, c = 1.13254( 1) nm, and β= 109.8001(3)°, and those of GdY(WO4)3 are a = 0.76175(1) nm, b = 1.13543(1) nm, c = 1.13496(2) nm, and bbbbbbbbbβwhile each rare-earth atom is surrounded by eight oxygen atoms. WO4 tetrahedra share their four vertices with REO8 (RE = Dy, Gd, or Y) trigondodecahedra and some REO8 trigondodecahedra share an edge with each other. The phase transition and the magnetic properties were investigated by differential thermal analysis (DTA) and dc superconducting quantum interference device (SQUID) magnetometer.     

Crystal structural refinement for NdAlSi

The compound NdAlSi was studied using X-ray powder diffraction technique and refined by the Rietveld method. The compound NdAlSi has tetragonal α-ThSiE-type structure, space group I41/amd （No. 141）, Z = 4, and the lattice parameters a = 0.41991（1） nm, c = 1.44916（3） nm. The Smith and Snyder figure of merit FN is F30= 103.1（36）. The R-factors of Rietveld refinement are Rp= 0.113 and Rwp= 0.148, respectively. The X-ray powder diffraction data is presented in this article.     

ISOTHERMAL SECTION OF Mg-Zn-La SYSTEM IN Mg RICH CORNER AT 350℃

Alloys of Mg-Zn-La system in Mg rich corner at 350℃ have been prepared in this study. Scanning electron microscopy （SEM）, electron probe microanalysis with energy dispersive X-ray spectroscopy （EPMA-EDS）, and X-ray diffraction （XRD） have been used to identify the phase equilibrium and the composition of each phase in the alloys. As a result, the isothermal section of Mg-Zn-La system in Mg rich corner at 350℃ has been determined. The result shows that, in addition to some binary phases, there exists a linear ternary compound called T-phase in Mg-Zn-La system at 350℃, in which the La content is about 8 at. pct ±0.4 at. pct and the Zn content is 8 at. pct- 48 at. pct. The T-phase has a C-centered orthorhombic crystal structure, and the lattice parameters are a=0.965-1.020 nm, b=1.121 1.142 nm, c=0.950-0.977 nm.