(K,Na)3La2(BO3)3固溶体系的晶体结构

本文合成了一系列的(K,Na)3La2(BO3)3硼酸盐,通过自发结晶得到了组分为K1.34,Na1.66La2(BO3)3的单晶.单晶X射线结构分析表明该晶体与Na3La2(BO3)3同构,并且当K+取代Na+的数量小于2/3时,晶体结构仍为Na3La2(BO3)3构型.该晶体的基本结构单元为孤立的(BO3)3-基团.一个单胞中含有6个BO3基团,其中两个沿c方向一致平行排列,而剩余的4个BO3基团的排列方向与c方向呈一定的角度,从而减小了BO3基团对非线性效应的贡献.粉末倍频测试该晶体的有效非线性系数约为KDP的2.4倍.此外,研究表明用适量的Rb+,Li+取代Na+时,固溶晶体结构也不发生改变.     

高温超导及GaN衬底材料(La,Sr)(Al,Ta)O3晶体的生长

用提拉法生长了高质量、大尺寸、具有混合钙钛矿结构的(La,Sr)(Al,Ta)O3晶体(LSAT),晶体尺寸达55mm×50mm.讨论了晶体生长有关工艺,并对晶体的完整性进行了初步研究.     

Magnetic, magnetocaloric, and lattice properties of the La(Fe x Si1 − x )13 ferromagnets

The magnetic and lattice properties of a sample of La(Fe_0.86Si_0.14)₁₃ ferromagnet have been measured. The influence that neutron irradiation has on the physical properties of this ferromagnet is studied. It is shown that the irradiation of this sample by a fluence of 3 × 10¹⁹ n/cm² increases the lattice constant a and the Curie temperature (T _C ) as the volume magnetostriction decreases. A model of ferromagnet is proposed which satisfactorily describes the dependence a(T) of the initial and irradiated samples and their magnetic properties. The temperature dependence of the change in entropy when switching the magnetic field on and off is calculated. It is established that the change in both the magnetic and lattice parts of the total entropy at the magnetic phase transition must be taken into account for La(Fe _x Si_{1 ? x} )₁₃ compounds.     

Na3La2(BO3)3的晶体结构

以Na2CO3-H3BO3-NaF为助熔剂,使用顶部籽晶法生长出Na3La2(BO3)3透明单晶.测定了Na3La2(BO3)3的晶体结构,该晶体属正交晶系,空间群:mm2(No.38),晶胞参数为a＝0.51580(10)nm,b=1.1350(2)nm,c=0.73230(15)nm,α＝β＝γ＝90°,V＝0.42871(15)nm3,密度:.053g/cm3.晶体结构中的硼氧基团是平面的BO3基团,BO3基团相互独立,且与Na(1)O6、Na(2)O8、Na(3)O6和La(1)O9配位多面体连结形成三维网络骨架结构.讨论了Na3La2(BO3)3的晶体结构与倍频效应的关系.     

水热LSS法制备La(OH)3 纳米晶

采用基于在水热合成的过程中发生于液相、固相和溶液相界面处的相扩散和分离机制的液相(Liquid)-固相(Solid)-溶液相(Solution)(LSS)法成功地制备出具有规则形状的La(OH)3纳米晶,主要研究了水热反应釜填充比、水热反应温度等工艺因素对La(OH)3纳米晶的晶粒尺寸及相组成的影响.采用X射线衍射仪、纳米粒度分析仪和透射电子显微镜对所制备的La(OH)3纳米晶进行表征.结果表明:所制备的La(OH)3由直径约为10～40nm的纳米晶组成,晶粒尺寸分布均匀;随着水热反应温度从120℃增加到220℃,La(OH)3纳米晶结晶程度提高,晶粒的平均尺寸从14nm增加到40nm;在60～80;范围内,水热反应釜填充比对La(OH)3纳米晶的粒度影响不大.     

(La,Y)掺杂AlN的电子结构和光学性质的第一性原理研究

采用基于密度泛函理论的平面波超软赝势方法对纯AlN、(La,Y)单掺杂以及La-Y共掺杂AlN 超胞进行几何结构优化,计算了稀土元素(La,Y)掺杂前后体系的能带结构、态密度和光学性质。结果表明:未掺杂的AlN是直接带隙半导体,带隙值为E_g=4.237 eV,在费米能级附近,态密度主要由Al-3p、N-2s电子轨道贡献电子,光吸收概率大,能量损失较大;掺杂后使得能带结构性质改变,带隙值降低,能带曲线变密集,总态密度整体下移;在光学性质中,稀土元素掺杂后均提高了静态介电常数、光吸收性能,增强了折射率和反射率,减小了电子吸收光子概率及能量损失;其中La-Y共掺体系变化得较为明显。     

Na3La9O3(BO3)8的晶体结构

以Na2CO3-H3BO3为助熔剂,用顶部籽晶法生长出Na3La9O3(BO3)8单晶.测定了Na3La9O3(BO3)8晶体结构,结果表明:该晶体属六方晶系,空间群:P62m,晶胞参数为a=b=0.89229(13)nm,c=O.87366(17)nm,α=β=90°,γ=120°,Z=1,V=0.60240(17)nm3,密度为5.066g/cm3.晶体结构中的硼氧基团是平面的BO3基团,BO3基团相互独立,通过与Na(1)O6、La(1)O9和La(2)O8的配位多面体连结形成层状结构,所有层平行于(001)面.描述了Na3La9O3(BO3)8晶体在非线性光学材料领域的应用前景.     

Synthesis and crystal structure of the heterometallic square-chain polythiometalate: {[W4Ag5S16]2 · [La(DEF)2(DMF)6][La(DEF)4(DMF)4]}n

The complex (NH₄)₂ WS₄ reacts with AgNO₃ and La(NO₃)₃·6H₂O in a mixture of DEF/DMF (DEF—N,N-diethylformamide), to give a new heterometallic square-chain polythiometalate {[W₄Ag₅S₁₆]₂·[La(DEF)₂(DMF)₆]·[La(DEF)₄(DMF)₄]}_n (1). 1 crystallizes in the monoclinic space group P2/c, a = 19.5534(8), b = 16.9552(6), c = 22.3479(9) Å, = 106.053(1)°, V = 7120.1(5) ų, and Z = 2. The anion polymeric chain of 1 can be regarded as an octanuclear cyclic cluster of [W₄Ag₄S₁₆]^4– fragments linked through Ag⁺ ions. The polymeric chain is extended through the parallel edges of the square unit. The mean W—Ag distance is 2.963(16) Å. The La³⁺ cations are coordinated by different solvent molecules, the average La—O bond of these large trivalent cations is 2.47(1) Å.     

Na3La2(BO3)3晶体生长及光谱特性

本文以起始摩尔比为1:1的Na2CO3:H3BO3,并添加5;质量分数的NaF为助熔剂,用顶部籽晶法生长出φ35mm×5mm的透明Na3La2(BO3)3单晶.该晶体属正交晶系,空间群:Amm2,晶胞参数为a=0.51580(10)nm,b=1.1350(2)nm,c=0.73230(15)nm,α=β=γ=90°.测量了Na3La2(BO3)3晶体在室温下的透过光谱,紫外截止波长约为200nm.该晶体常温下稳定,不吸潮,但却易溶于稀酸.     

Structure of [La(NO3)3(OH2)2(OHMe)(bipy)]·15-crown-5

[La(NO₃)₃(OH₂)₂(OHMe)(bipy)·15-crown-5 is monoclinic,P2_t/n, witha=11.239(6),b=19.302(7),c=14.458(8) , =92.47(5)°, andD _calc=1.63 g cm^–3 forZ=4. In the complex, two nitrogen atoms (from bipy) and nine oxygen atoms (six from three bidentate nitrate anions, two from water molecules, and one from a methanol molecule) coordinate to the La(III) ion forming a coordination polyhedron which approximates a skewed trigonal prism with an interpenetrating pentagon. The coordinated methanol and water molecules donate hydrogen bonds to the oxygen atoms of the crown ether forming polymeric hydrogen bonded chains which propagate along theac diagonal in the unit cell.     

Synthesis, spectral, and single crystal X-ray structural studies on (2,2′-bipyridyl)bis(dimethyldithiocarbamato) zinc(II) and (1,10-phenanthroline) bis(dimethyldithiocarbamato)zinc(II)

Synthesis, spectral, and single crystal X-ray structural studies on (2,2-bipyridyl)bis (dimethyldithiocarbamato)zinc(II) (1) and (l,10-phenanthroline)bis(dimethyldithiocarbamato)zinc(II) (2) complexes are reported in this paper. The complex (1) crystallizes in the orthorhombic lattice, space group Pcca, a = 18.456(3), b = 6.529(2), and c = 17.092(2) Å. The complex (2) crystallizes in the monoclinic space group C2/c, a = 13.372(2), b = 13.850(2), c = 24.680(3) Å, and = 102.71(4)°. IR spectra of the complexes (1) and (2) show the thioureide (C-N) bands at 1489 and 1510 cm^–1, respectively, which are lower than the value observed for the parent bisdithiocarbamate. Reduction in the thioureide stretching frequency is due to the increase in coordination around the zinc ion and the resultant increase in electron density. Thermal studies indicate that the 1,10-phenanthroline adduct is marginally more stable than the other complex. X-ray crystal structures of the two adducts show them to be octahedrally coordinated and monomeric in nature. The Zn-S distances are longer than those observed in the parent bisdithiocarbamate. The thioureide C-N bond distances in (1) and in (2) indicate the partial double bond character. The most important structural changes as a result of the adduct formation are observed in the Zn-S bond distances and S-Zn-S bond angles, in terms of very significant increases in Zn-S bond distances and reductions in S-Zn-S angles, compared to the parent bisdithiocarbamate. The observed changes are indicative of a strong steric force in operation in the adducts rather than electronic effects.     

(La0.75Sm0.25)2Zr2O7陶瓷的热导率

以Sm2O3、La2O3和ZrO2为原料,用固相反应法制备了(La0.75Sm0.25)2Zr2O7陶瓷材料.采用XRD和FT-IR技术研究了试样的相结构,用SEM分析了试样的微观组织结构,采用激光脉冲法测量试样的热导率.结果表明,所制备的陶瓷材料具有焦绿石晶体结构,其组织结构致密,晶粒大小均匀,晶界清晰.由于La3+和Sm3+质量和离子半径的差别, (La0.75Sm0.25)2Zr2O7具有比La2Zr2O7更低的热导率.其热导率明显低于现役的YSZ陶瓷,可用作新型热障涂层表面陶瓷层候选材料.     

钙钛矿型层状化合物K_2Ln_2Ti_3O_(10)(Ln=La,Pr,Sm,Eu,Gd)X射线衍射晶体结构分析

固相反应法合成了具有钙钛矿型层状的化合物K_2Eu_2Ti_3O_(10) 和K_2Gd_2Ti_3O_(10) ,利用X射线粉晶衍射仪对镧系元素的钙钛矿型层状化合物K_2Ln_2Ti_3O_(10) (Ln=Eu,Gd)进行结构分析,获得其X射线粉晶衍射数据.X射线衍射分析结果表明:K_2Ln_2Ti_3O_(10) (Ln= La,Pr,Sm,Eu,Gd )为四方晶系,空间群I4/mmm.并得到其晶胞参数及其镧系元素的钙钛矿型层状化合物K_2Ln_2Ti_3O_(10) 晶体结构变化规律.     

Structure of bis(O,O′-diisopropyldithiophosphato-S,S′) (1,10-phenanthroline-N1,N10)zinc(II) complex, [Zn(phen)(S2P(OiPr)2)2]

The crystal and molecular structure of [Zn(phen)(S₂P(OiPr)₂)₂] (Phen = 1,10-phenanthroline) has been determined by X-ray crystallography. It crystallizes in the Monoclinic system, space group C2/c, with lattice parameters a = 19.315(4), b = 10.438(2), c = 16.567(3)Å, = 102.89 (3)°, and Z = 4. The complex has C₂ symmetry. The coordination geometry of each Zn atom, by two S atoms from two (O,O-diisopropyldithiophosphato) anions and by two N atoms from phenanthroline ligand, is that of a slightly distorted tetrahedron [Zn—S 2.2914(8)Å Zn—N 2.111(2)Å]. The Zn···S distances to the noncoordinated S atoms are long: 3.5276 Å, which are indicated that there are much weaker interactions between them.     

Synthesis, crystal structure, and spectroscopy of (azido-N1)bis(2,2′-bi-imidazoline)copper(II) perchlorate

The compound [Cu(biz)₂(N₃)](ClO₄) (biz = 2,2-bi-imidazoline) has been synthesized and characterized by X-ray crystallography and infrared spectroscopy. In addition, EPR and magnetic measurements have been performed. The compound crystallizes in the monoclinic space group P2₁/c, with a = 9.2716(2), b = 27.6454(4), c = 7.4285(1) Å, = 102.1417(6)°, V = 1861.46(5) ų, and Z = 4. The coordination geometry around the Cu(II) ion is distorted square pyrimidal, with 4 nitrogen atoms of 2 bis-chelating ligand molecules in the basal plane and one nitrogen of the azide molecule in the apical position. The perchlorate ion is noncoordinating. In the infrared the vibrations of the coordinated azide anion are observed at 2050, 1286, and 620 cm^–1, while the vibrations of the free perchlorate anion are observed at 1071, 1035, and 919 cm^–1; Cu—N vibrations are observed at 418 and 336 cm^–1. The molecules are connected in the lattice via relatively strong hydrogen bonding between the N—H groups at the back of the biz ligand and the N1 and N3 atoms of the azide ligand forming layers. No intermolecular magnetic interaction was observed for this compound.     

Crystal structures of bis(cyanido)bis(N,N′-diethylthiourea-κS) mercury(II) and bis(cyanido)bis(N,N′-dipropylthiourea-κS) mercury(II)

Two mercury(II) complexes containing cyanide and, N,N′-diethylthiourea (detu) and N,N′-dipropylthiourea (dprtu) ligands, [(detu)₂Hg(CN)₂] (1) and [(dprtu)₂Hg(CN)₂] (2), respectively, have been prepared and characterized by X-ray crystallography. In the both complexes Hg atom lies on a 2-fold rotation axis, and is coordinated to the sulfur atoms of two thiourea ligands and to two cyanide carbon atoms. Both have a distorted tetrahedral environment with bond angles about the Hg atoms in the range of 93.41(4)°–146.75(19)°. In the crystal structures symmetry related molecules are linked via N-H-N hydrogen bonds resulting in the formation of a two-dimensional network in 1, while in 2 a double stranded one-dimensional chain is formed.     

Structure,bonding, and magnetic behavior of bis(μ-chloro)-and (μ-bromo)-bridged Cu(II) dimers

It has been previously reported that dimeric compounds of the general formula [L₃Cu(II)]₂(-Cl)₂ exhibit a correlation between their magnetic coupling constantJ and the bridging Cu-Cl-Cu angle. A full survey of the published structural and magnetic data on these compounds confirms this correlation but leads to the conclusion that its physical significance is questionable. EHMO calculations on Cu₂Cl ₈ ^4– and its bromo analog show that the molecular orbitals responsible for the magnetic behavior of the dimers are not the orbitals responsible for the bonding interactions in these dimers. Therefore, they are very weakly affected by variations of the molecular structure, and no significant correlation betweenJ and any of the structural parameters is theoretically predicted. However, this situation changes when the coordination around the Cu atoms is strongly and dissymmetrically pyramidalized.     

微波加热制备含稀土(La2O3)矿渣微晶玻璃研究

利用矿渣制备微晶玻璃是提高矿产资源利用率的主要形式之一。本文以白云鄂博尾矿为原料,采用微波一步法制备了CaO-MgO-Al₂O₃-SiO₂(CMAS)系辉石相矿渣微晶玻璃。选择835 ℃作为晶化温度,研究了微波加热对微晶玻璃析晶行为和微观组织的影响。以La₂O₃作为研究变量探讨了La₂O₃添加对矿渣微晶玻璃析晶行为的作用。与传统的热处理制度相比,微波加热可以在较短的时间内达到较高的析晶效果。同时La₂O₃的添加促进了晶粒细化。由拉曼光谱分析,La离子添加会导致玻璃网络中桥氧的增多,促进了辉石相析晶。在La的添加量为4%(质量分数)时硬度最高,达到了829.22 MPa。     

含NiTi阻挡层的硅基(La0.5Sr0.5)CoO3/Pb(Zr0.4Ti0.6)O3/(La0.5Sr0.5)CoO3铁电电容器异质结

应用磁控溅射法制备的非晶NiTi薄膜作阻挡层,在Si (100)衬底上构造了(La0.5Sr0.5)CoO3/ Pb(Zr0.4Ti0.6)O3/(La0.5Sr0.5)CoO3(LSCO/PZT/LSCO)铁电电容器异质结,研究了Pb(Zr0.4Ti0.6)O3铁电薄膜的结构和物理性能.实验发现LSCO/PZT/LSCO铁电电容器具有良好的电学性能,在417kV/cm的驱动场强下,PZT铁电电容器具有较低的矫顽场强(125kV/cm)和较高的剩余极化强度(19.0μC/cm2),良好电容-电压特性(C-V)和保持特性,铁电电容器经过1010次反转后,极化强度没有明显下降,表明了非晶NiTi薄膜可以用作高密度硅基铁电存储器的扩散阻挡层.     

The crystal structure and supramolecular chain of [La(NO3)3(OH2)2(phen)] ⊙ 15-crown-5

[La(NO₃)₃(OH₂)₂(phen)] · 15-crown-5 is hexagonal,P6₅, witha=10.955(2),c=43.769(9), andD _calc =1.668 g cm^–3 for Z=6. In the complex, two nitrogen atoms (from phen) and eight oxygen atoms (six from three bidentate nitrate anions and two from water molecules) are coordinated to the central La(III) ion, forming a coordination polyhedron which is approximately a bicapped square antiprism. The coordinated water molecules donate hydrogen bonds to the oxygen atoms of the crown ether, forming polymeric hydrogen bonded chains which wrap helically along the unit cell directionc.