Fe_x(In_2O_3)_(1-x)磁性颗粒膜的结构及光学性质

用射频溅射法制备了金属 /半导体 Fex(In2 O3) 1-x 颗粒膜。实验结果表明 :纳米尺度的Fe颗粒比较均匀地分布在非晶态母体In2 O3 中。退火可使In2 O3 晶化。该样品在室温下表现出超顺磁驰豫 ,符合Langevin方程。光学测量表明 :嵌Fe的磁性颗粒膜 ,其电子的带间跃迁由In2 O3 的直接跃迁变为间接跃迁 ,基本吸收边红移 ;随磁性增强 ,局域态尾变宽 ,带隙变窄     

金属掺杂对In2O3薄膜光学性质的影响

研究了射频溅射法制备的金属／半导体类型颗粒膜的光学特性。通过样品透射谱分析，发现金属Fe的掺杂使半导体In2O3的带间跌迁由直接跃迁变为间接跃迁；随Fe所占体积份数的增加，局域态尾变宽，带隙变窄。这是由于掺入Fe颗粒后。母体材料与金属颗粒的界面处表面态增多，以及母体材料的非晶化引起的。     

制备条件和退火处理对Fex/(In2O3)1-x颗粒膜结构、磁性及巨磁电阻的影响

用射频溅射法成功制备了金属／半导体型颗粒膜Fex／(In2O3)1-x实验结果表明样品的微结构、磁性和巨磁电阻效应受制备条件(如本底真空度、衬底温度、溅射电压等)以及热退火处理的强烈影响。较高的衬底温度有利于基体In2O3的晶化和Fe颗粒的成长。适当的热退火能促使Fe颗粒生长，使晶格畸变减小，从而改善膜的微结构。室温下，磁性测量表明样品具有超顺磁性，符合朗之万方程。高温退火后，颗粒的大小已超过单畴粒子的临界尺寸，引起矫顽力下降。     

Fe／In2O3磁性颗粒膜的光学特性

研究了射频溅射法制备的磁性颗粒膜的光学特性。发现在Ｉｎ２Ｏ３母体材料中嵌入Ｆｅ颗粒的磁性颗粒膜中，电子的带间跃迁由Ｉｎ２Ｏ３的直接跃迁变为间接跃迁，基本吸收边变平；随磁性粒子所占体积分数的增加，局域态尾变宽，带隙交窄。这是由于嵌入Ｆｅ颗粒后，母体材料与磁性颗粒的界面积增加，具有了较多的表面态，以及母材料的非晶化引起的。     

纳米Fe-ZnSe颗粒膜的光学特性

研究了射频溅射法制备的纳米"铁磁金属一半导体基体"Fex(ZnSe)1-x颗粒膜的光学特性.透射光谱测量结果表明,当Fe体积分数为35%时,颗粒膜样品的可见光透过率达到50%以上.研究发现,在ZnSe薄膜基体中嵌入纳米铁颗粒的Fe-ZnSe颗粒膜中,电子的带间跃迁为直接跃迁,其带隙随着Fe在颗粒膜中所占体积分数的增加而变宽.     

Fe3O4@Au@Ag复合纳米材料的制备及SERS研究

用化学共沉淀法制备Fe3O4,用静电吸附法制备Fe3O4@Au复合磁性纳米材料,用种子生长法制备出Fe3O4@Au@Ag复合磁性纳米材料。利用紫外一可见吸收光谱研究复合磁性纳米颗粒的光谱特性,以结晶紫为探针分子检测磁性纳米颗粒的表面增强拉曼散射光谱。实验结果表明：复合磁性纳米颗粒既具有磁性又具有贵金属光谱特性;复合磁性纳米颗粒能很好地改善Fe3O4磁性纳米颗粒的表面增强拉曼散射活性。     

酸碱度对纳米Fe_3O_4磁性流体性能的影响

采用化学共沉淀法制备纳米Fe3O4磁性颗粒,并用油酸钠对其进行包覆改性,以煤油为基液制备出煤油基Fe3O4磁流体。对比分析了pH值=5和10.5条件下油酸钠包覆的Fe3O4磁性颗粒的性能差异,得出油酸钠在pH值=5时可以更好地包覆在Fe3O4磁性颗粒表面,其饱和磁化强度为58.0A·m2/kg,在此基础上制备出的磁流体的饱和磁化强度为20.2A·m2/kg,并且Fe3O4磁性颗粒分散较均匀。而油酸钠在pH值=10.5时包覆的Fe3O4磁性颗粒,其饱和磁化强度虽然高一些(67.8A·m2/kg),但制备出的磁流体稳定性较差,出现较为明显的沉降现象。     

Fe304／Au复合纳米材料的制备及SERS研究

采用化学共沉淀法制备Fe3O4,通过对Fe3O4的表面处理后,将纳米金组装在Fe3O4表面,制备Fe3O4／Au复合磁性纳米材料。利用透射电子显微镜（TEM）对复合磁性纳米材料的形貌进行了表征,通过紫外一可见吸收光谱和拉曼光谱仪对磁性纳米材料的表面增强拉曼散射光谱进行表征研究,采用铷硼磁铁对磁性纳米材料的磁性进行初步研究。实验结果表明：复合磁性纳米颗粒既具有磁性又具有贵金属光谱特性;纳米金能很好地改善Fe3O4磁性纳米颗粒的表面增强拉曼散射活性。     

无水乙醇对双层油酸包覆结构中物理吸附层的影响

研究了无水乙醇洗涤次数对油酸包覆的Fe3O4磁性纳米颗粒表面包覆结构的影响。采用FT-IR和TGA联合表征了油酸包覆的Fe3O4磁性纳米颗粒经过无水乙醇洗涤前后表面包覆结构的变化,采用TEM观察了油酸包覆后Fe3O4磁性纳米颗粒的形貌。实验结果表明经过无水乙醇5次洗涤后,油酸包覆的Fe3O4磁性颗粒为双层包覆结构;经过无水乙醇20次洗涤后,无水乙醇将双层油酸包覆结构中的物理吸附层洗掉,造成双层油酸包覆的Fe3O4磁性颗粒演变为单层包覆结构。     

Fe_3O_4/Au复合磁性纳米颗粒的制备及其表征

首先通过化学共沉淀法制备出Fe3O4磁性纳米颗粒,考察了表面活性剂的用量、碱的用量、陈化时间以及三价铁与二价铁的摩尔比等因素对Fe3O4纳米颗粒性能的影响。制备出饱和磁化强度为73.85A.m2/kg、粒径大小为10nm以下的Fe3O4纳米颗粒。在此基础上,制备出Fe3O4/Au复合纳米颗粒,通过VSM、TEM、XRD、XPS对产物进行了表征,研究了HAuCl4的用量、还原剂的种类、硅烷偶联剂以及包金之前的Fe3O4纳米颗粒对复合颗粒的影响,结果表明所制得的Fe3O4/Au复合磁性纳米颗粒包覆良好,粒径大小为50～200nm,饱和磁化强度为10.08A.m2/kg。     

K2(Rb2,Cs2,Tl2)TeBr6(I6) and Rb3(Cs3)Sb2(Bi2)Br9(I9) perovskite compounds

We systematize available experimental data on the crystal structure of the ternary halides K₂(Rb₂,Cs₂,Tl₂)TeBr₆(I₆) and Rb₃(Cs₃)Sb₂(Bi₂)Br₉(I₉), analyze the general trends in the properties of their single crystals, and examine the key features of the physicochemical interaction in related systems.     

Flux growth of single magnetic sublattice antiferromagnetic garnets Ca3 Fe2 Ge3 O12 and Ca3 Mn2 Ge3 O12

Magnetic single crystals garnets Ca₃ X₂ Ge₃ O₁₂ with X = Mn³⁺ or Fe³⁺ containing Ca²⁺ and Ge⁴⁺ are of great interest due to the rise of an antifer-romagnetic order in one definite octahedral site. The optimal conditions for obtaining single magnetic-sublattice garnets of large size (1 cm in diameter) have been analyzed. Two groups of solvents have been tested: Bi₂ O₃ or PbO based flux. The best results were obtained with PbO flux and starting composition : % Moles 44 PbO 1b 35 GeO₂ 1b 15 CaO 1b 6 X₂ O₃.     

Syntheses and structures of Ta2(WO2)0.87H0.26(PO4)4 and Ta2(MoO2)(PO4)4

Tantalum hydrogen phosphate, β-TaH(PO₄)₂, has a three-dimensional structure that is stable to remarkably high temperature (∼600 °C) presumably due to the presence of strong hydrogen bonds. Impedance measurements indicate a low conductivity, 2.0 × 10⁻⁶ S/cm at 200 °C in 5% H₂. In further studies aimed at enhancing the conductivity by aliovalent doping, we have investigated systematically the synthesis of compounds in the TaH(PO₄)₂-W₂P₂O₁₁ system at 380 °C. As a result, a new phase, Ta₂(WO₂)_0.87H_0.26(PO₄)₄, was identified and subsequently the molybdenum analog Ta₂(MoO₂)(PO₄)₄ was also prepared. The structures were determined by single crystal X-ray diffraction techniques. The structures of Ta₂(WO₂)_0.87H_0.26(PO₄)₄ and Ta₂(MoO₂)(PO₄)₄ can be formally derived from the structure of β-TaH(PO₄)₂ by the replacement of two P-OH protons with an MO₂²⁺ (M = Mo and W) group together with a change in the orientation of some phosphate tetrahedra.     

(K0.44,Na0.52,Li0.04) (Nb0.84,Ta0.10,Sb0.06)O3 Ferroelectric Ceramics

Recent progress in (K_0.44,Na_0.52,Li_0.043-based ceramics (KNN) with special emphasis on (K_0.44,Na_0.52,Li_0.040.84,Ta_0.10,Sb_0.06))O₃ (KNN-LT-LS) is reviewed concisely. The base KNN and its compositional derivatives are analyzed in terms of dopant-property relationships, which are then extended to the ternary derivatives. The effects of processing conditions such as humidity, precursor purity, and oxygen partial pressure during sintering are elaborated on from a phenomenological perspective. It is also shown that the spontaneous polarization is sensitive to the processing route chosen for synthesis (mixed oxide versus perovskite routes). Special attention is devoted to the discussion of the morphotropic phase boundary (MPB) dilemma in the KNN-LT-LS system, where it is shown that the origin of high piezoelectric activity is actually due to a polymorphic transition at room temperature. It is shown that prototype transducers based on pure and 1 mol% Ba²⁺ doped KNN-LT-LS exhibit performance metrics comparable to those fabricated using PZT-5H. Overall, KNNLT- LS ceramics show great promise for lead-free applications, although issues such as temperature dependence of properties and strong sensitivity to processing conditions remain as the 2 major challenges.     

Preparation of (NH4)Zr2(PO4)3 and HZr2(PO4)3

(NH₄)Zr₂(PO₄)₃ has been prepared, hydrothermally, from α-zirconium phosphate in three different ways; (1) from amine intercalates at 300°C, (2) from mixtures of ZrOCl₂·8H₂O in excess (NH₄)H₂PO₄ and (3) reaction of NH₄Cl with Zr(NaPO₄)₂. Ammonium dizirconium triphosphate is rhombohedral with a = 8.676(1) and $\text{c}\text{= 24.288(5)}\text{A}\text{?}$. It decomposed on heating to HZr₂(PO₄)₃. Below 600°C a complex, as yet unindexed, X-ray pattern was obtained. A very similar X-ray pattern was obtained by washing LiTi_0.1Zr_1.9(PO₄)₃ with 0.3N HCl. Heating this phase or NH₄Zr₂(PO₄)₃, above 600°C resulted in the appearance of a rhombohedral phase of HZr₂(PO₄)₃ with cell dimensions a = 8.803(5) and $\text{c}\text{= 23.23(1)}\text{A}\text{?}$. The protons were not completely removed until about 1150°C. Decomposition of (NH₄)Zr₂(PO₄)₃ at 450°C yielded an acidic gas whereas at 700°C NH₃ was evolved. A possible explanation for this behavior is presented.     

Dielectric properties of Pb3 (PO4)2 | Pb3 (AsO4)2

The dielectric constants of Pb₃ (PO₄)₂ | Pb₃ (AsO₄)₂ at room temperature are intrinsic and fulfill the Lyddane - Teller - Sachs relation. At higher temperatures the specific conductivity increases with an activation energy of 0.56 eV leading to Maxwell - Wagner polarization effects thereby increasing the effective dielectric constant. Corresponding peaks in ∈' (T) are extrinsic and not attributed to structural phase transformations.     

Bi3(FeO4)(MoO4)2 and Bi3(GaO4)(MoO4)2 - new compounds with scheelite related structures

The title compounds have been prepared for the first time. They have monoclinic structures related to the scheelite (CaWO₄) structure, and they represent the first example of trivalent cations on tetrahedral sites of the scheelite structure. A superstructure is observed due to an ordering of the cations on the tetrahedral sites.     

Hydrothermal Crystallization in the Systems La2(CO3)3 ? 6H2O-CaCO3(BaCO3)-R-H2O (R = Na2CO3, K2CO3, NaHCO3, KHCO3, NaCl, NH4Cl, CO(NH2)2)

Crystallization in the systems La₂(CO₃)₃ ⋅ 6H₂O-CaCO₃(BaCO₃)-R-H₂O (R = Na₂CO₃, K₂CO₃, NaHCO₃, KHCO₃, NaCl, NH₄Cl, CO(NH₂)₂) was studied under hydrothermal conditions (400–450°C). The solid reaction products were found to contain LaOHCO₃ and NaLa(CO₃)₂. Detailed thermal decomposition schemes were proposed for these phases, and their lattice parameters were refined. __________ Translated from Neorganicheskie Materialy, Vol. 41, No. 11, 2005, pp. 1366–1372. Original Russian Text Copyright ? 2005 by Nikol'skaya, Dem'yanets.     

Direct observation of ferroelasticity in Pb3(PO4)2  Pb3(VO4)2

Ferroelasticity has been established in the room temperature phase of Pb₃(P_xV_1-xO₄)₂, (x ≥ 0.8). The coercitive stress and the spontaneous strain have been determined and found to be 1.6 bars and ca. 3.5 · 10^?4 respectively. The effect of domain switching on double refraction and Raman spectra is clearly brought out.     

Crystal Structure of (H3O)6[(UO2)5(SeO4)8(H2O)5](H2O)5

Crystals of (H₃O)₆[(UO₂)₅(SeO₄)₈(H₂O)₅](H₂O)₅ were prepared from aqueous solutions by evaporation. The crystal structure [monoclinic system, space group P2₁/m, a = 13.835(2), b = 13.4374(16), c = 14.310(3) Å, β = 108.004(14)°, V = 2530.1(7) Å ³] was solved by the direct method and refined to R ₁ = 0.090 for 4409 reflections with |F _hkl ≥ 4σ|F _hkl |. The structure is based on [(UO₂)₅(SeO₄)₈(H₂O)₅]⁶⁻ layers arranged parallel to the (101) plane; these layers have a unique topological structure. The U(1)O₆(H₂O) and U(3)O₆(H₂O) linked through selenate groups form chains running along [ [`1]\bar 1 01] direction. The chains are combined in layers by U(2)O₆(H₂O) bipyramids. The layers are linked with each other by hydrogen bonds through the H₂O and H₃O⁺ groups located between the layers.