碳酸镧分离富集DNA的研究

通过紫外-可见分光光度法测定了碳酸镧吸附前后溶液中的DNA含量,并计算了DNA的吸附率.通过X射线光电子能谱(XPS)与X射线衍射(XRD)分析了吸附DNA前后固相的变化.结果表明,碳酸镧对DNA有较强的吸附作用,且该过程对碳酸镧晶型未产生明显影响.通过对吸附条件的考察,发现DNA的吸附率随pH值升高而降低.最后通过磷酸二氢钾作为洗脱液将吸附的DNA回收,洗脱液中镧离子含量低于0.1×10~(-6)mol/L,对DNA的后期使用无污染.     

La3OCl[AsO3]2: Ein Lanthan‐Oxidchlorid‐Oxoarsenat(III) mit “lone‐pair”‐Kanalstruktur

La₃OCl[AsO₃]₂: A Lanthanum Oxide Chloride Oxoarsenate(III) with a “Lone‐Pair” Channel Structure La₃OCl[AsO₃]₂ was prepared by the solid‐state reaction between La₂O₃ and As₂O₃ using LaCl₃ and CsCl as fluxing agents in evacuated silica ampoules at 850 °C. The colourless crystals with pillar‐shaped habit crystallize tetragonally (a = 1299.96(9), c = 558.37(5) pm, c/a = 0.430) in the space group P4₂/mnm (no. 136) with four formula units per unit cell. The crystal structure contains two crystallographically different La³⁺ cations. (La1)³⁺ is coordinated by six oxygen atoms and two chloride anions in the shape of a bicapped trigonal prism (CN = 8), whereas (La2)³⁺ carries eight oxygen atoms and one Cl^? anion arranged in the shape of tricapped trigonal prism (CN = 9). The isolated pyramidal [AsO₃]^3? anions (d(As–O) = 175–179 pm) consist of three oxygen atoms (O2 and two O3), which surround the As³⁺ cations together with the free, non‐binding electron pair (lone pair) Ψ¹‐tetrahedrally (?(O–As–O) = 95°, 3×). One of the three crystallographically independent oxygen atoms (O1), however, is exclusively coordinated by four (La2)³⁺ cations in the shape of a real tetrahedron (d(O–La) = 236 pm, 4×). These [(O1)(La2)₄]¹⁰⁺ tetrahedra form endless chains in the direction of the c axis through trans‐edge condensation. Empty channels, constituted by the lone‐pair electrons of the Cl^? anions and the As³⁺ cations in the Ψ¹‐tetrahedral oxoarsenate(III) anions [AsO₃]^3?, run parallel to [001] as well.     

对乙酰基偶氮氯膦与镧显色反应的研究及应用

研究了对乙酰基偶氮氯膦与镧的显色反应 ,在 0 .2 mol/L 盐酸介质中 ,有乙醇及吐温 - 80存在时 ,生成3∶ 1紫色络合物。 λmax=6 75 nm,ε=7.33× 1 0 4 L· mol- 1· cm- 1。采用双波长法 ,以 5 30 nm为参比波长 ,6 75 nm为测定波长 ,ε=9.2 0× 1 0 4 L· mol- 1· cm- 1 ,镧含量在 0— 37.5 μg/2 5 m L范围内符合比耳定律。本法用于电子工业钛酸镧烧结中游离氧化镧的测定 ,结果令人满意。     

铕(Ⅲ)激活的磷酸镧发光性质研究

LaPO₄:Eu³⁺的发射光谱包含较强的Eu³⁺⁵D_o→⁷F₁跃迁发射和较弱的⁶D₁→⁷F₁跃迁发射。主发射峰583nm,对应于Eu³⁺5D_o→⁷F₁跃迁.通过对Eu³⁺的两种跃迁发射强度及荧光寿命和Eu³⁺浓度关系的测定和理论分析,探讨了发光中心Eu³⁺离子同的交叉弛豫和能量迁移机理。     

KBr-RE(La,Sm)Br3-13%HBr-H2O四元体系25℃时的相平衡研究

Meyer在研究K。REBr。（RE一La,Sin）的结构及热力学性能时,引用文献的方法合成了2：1型化合物见s．其具体反应机理尚未明确表示．根据文觎',合成2：1型化合物CSZLUCI。分两步：第一步是LtJ;03与CSCI在氢氯酸介质中反应,生成2：1型含结晶水的中间体CS入llCI;·H20;第二步是中间体在HCI气氛下的高温脱水反应．反应如下：HC＊＊;HCI;＊ISOOC4CSCI＋l。LI,O。、ZCS,LSCI。·H,O、ZCS,LllCI。－H人）由上述反应过程可见,中间体的形成实际上应是LLICI。与CSCI在HCI介质中反应的生成物．那么,Meye…     

镧(Ⅲ)-邻氯苯氧乙酸配合物的合成及性质

本文以邻氯苯氧乙酸（ＨＬ）为配体,合成了与稀土Ｌａ３＋离子的二元固体配合物ＬａＬ３Ｈ２Ｏ。并对该配合物进行了元素分析、摩尔电导、ＩＲ、ＵＶ、ＴＧ－ＤＴＡ、１ＨＮＭＲ等的测试分析。该配合物属螯合双齿配位。     

镧对镝-磺基水杨酸配合物荧光增强效应的研究和应用

本文研究发现,三价稀土离子Ｌａ３＋的存在对二元配合物Ｄｙ３＋－磺基水杨酸（ＳＳＡ）体系具有强烈的荧光增强效应。在常温条件下,研究了Ｌａ３＋参与下Ｄｙ３＋－ＳＳＡ体系的荧光特性、形成条件和影响因素,结果表明,Ｌａ３＋可使Ｄｙ３＋－ＳＳＡ体系荧光增强１００倍。在最佳条件下,Ｄｙ的浓度在３．０×１０－７～１．０×１０－５ｍｏｌ／ｄｍ３范围内与荧光强度成线性关系,检测限达到８．０×１０－８ｍｏｌ／ｄｍ３。利用该体系测定了合成稀土样品和包头稀土标准样品,结果满意,回收实验的回收率为９９．３％±０．１％。     

The effect of oxygen vacancy on the oxide ion mobility in LaAlO3-based oxides

The electrical property of (La_1−xSr_x)_1−z(Al_1−yMg_y)O_3−δ (LSAM; x≤0.3, y≤0.15 and z≤0.1) was measured using the DC four-probe method as a function of temperature (500–1000°C) and oxygen partial pressure (1–10⁻²² atm). Among LSAMs, (La_0.9Sr_0.1)AlO_3−δ showed the highest ionic conductivity, σ_i=1.3×10⁻² S cm⁻¹ at 900°C. A simultaneous substitution at A and B sites or A site deficiency is expected to create larger oxygen vacancy and higher ionic conductivity. However, it showed a negative effect. The effect of the vacancy increase did not effect monotonously the ionic conductivity. It was found that the concentration of oxygen vacancy, [V_O], influences not only the oxide ion conductivity, σ_i, but also the mobility, μ_v, of [V_O]. These properties exhibit a maximum at around [V_O]=0.05. With the increase in [V_O], the activation energy, E_a, of the ionic conduction dropped from 1.8 to ca. 1.0 eV at [V_O]=0.05 and became almost constant at [V_O]>0.05. The dependency of the pre-exponential term, μ⁰_v, and E_a on [V_O] was analyzed and their effect on μ_v and σ_i was discussed with respect to crystal structure and defect association. It was estimated that the crystal structure mainly governs these properties. The effect of defect association could not be ignored but is considered to be a complicated correlation.     

Synthesis and Crystal Structure of Rubidium Lanthanum Tetraacetate,RbLa(CH3COO)4

The anhydrous rubidium tetraacetato lanthanate, RbLa(CH₃COO)₄, is obtained together with Rb₂La(CH₃COO)₅(H₂O) as colourless single crystals from a 1 : 2 mixture of Rb₂CO₃ and La(CH₃COO) · 1.5 H₂O in acetic acid by slow evaporation. The crystal structure [orthorhombic, Pnnm, Z = 2, a = 1242.0(3), b = 1650.1(4), c = 698.0(4) pm, R = 0.028, R_w = 0.071] contains La³⁺ nine coordinate by oxygen atoms of six acetate ligands. The polyhedra are connected to dimers and further to double chains running parallel to [001]. These [La(CH₃COO)₄]^– double chains are surrounded by four like double chains and connected by Rb⁺ ions that are seven coordinate by oxygen atoms.     

La2Si2O7 im I—Typ: Gemäß La6[Si4O13][SiO4]2 kein echtes Lanthandisilicat

I‐Type La₂Si₂O₇: According to La₆[Si₄O₁₃][SiO₄]₂ not a Real Lanthanum Disilicate In attempts to synthesize lanthanum telluride silicate La₂Te[SiO₄] (from La, TeO₂, SiO₂ and CsCl, molar ratio: 1 : 1: 1 : 20, 950 °C, 7 d) or fluoride‐rich lanthanum fluoride silicates (from LaF₃, La₂O₃, SiO₂ and CsCl, molar ratio: 5 : 2 : 3 : 17, 700 °C, 7 d) in evacuated silica tubes, colourless lath‐shaped single crystals of hitherto unknown I‐type La₂Si₂O₇ (monoclinic, P2₁/c; a = 726.14(5), b = 2353.2(2), c = 1013.11(8) pm, β = 90.159(7)°) were found in the CsCl‐flux melts. Nevertheless, this new modification of lanthanum disilicate does not contain any discrete disilicate groups [Si₂O₇]^6‐ but formally three of them are dismutated into one catena‐tetrasilicate ([Si₄O₁₃]^10‐ unit of four vertex‐linked [SiO₄]^4‐ tetrahedra) and two ortho‐silicate anions (isolated [SiO₄]^4‐ tetrahedra) according to La₆[Si₄O₁₃][SiO₄]₂. This compound can be described as built up of alternating layers of these [SiO₄]^4‐ and the horseshoe‐shaped [Si₄O₁₃]^10‐ anions along [010]. Between and within the layers the high‐coordinated La ³⁺ cations (CN = 9 ‐ 11) are localized. The close structural relationship to the borosilicates M₃[BSiO₆][SiO₄](M = Ce ‐ Eu) is discussed and structural comparisons with other catena‐tetrasilicates are presented.