Ab Initio Study on The Influence of Spin State upon Bonding and Interaction in Fe-COBondCovalenciesinR2BaCuO5(R=Sm,Gd,Dy,Ho,Y,Er,Tm,Yb,Lu)

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MO-RE2O3-B2O3(M=Mg,Ca,Sr,Ba;RE=La,Eu,Gd)玻璃的发光性质

在空气中采用高温固相反应方法合成的17MO－（8-x-y)-75B2O3-xGd2O3(MLBEG,M-Mg,Ca,Sr,Ba)玻璃，在紫外光（λex=350nm)激发下发射蓝光和红光，在绿色光（λex=532nm)激发下发射红光，电子自旋共振谱研究表明玻璃体系中有Eu^2 离子存在，蓝色区的宽带发射是Eu^2 离子的5d-4f跃迁发射：红色区的窄带发射是Eu^3 离子的5Do-7FJ(J=1,2,3,4)跃迁发射，发现玻璃中的碱土金属离子对Eu^3 /Eu^2 离子的比例有很大影响，选择不同的碱土金属离子可以调节玻璃蓝色光和红色光的相对发射强度，MLBEG玻璃的发光性质可用于转换太阳能，增强植物的光合作用。     

RBa2Cu4O8(R=Dy, Ho, Er, Tm, Yb)和Y2Ba4Cu7O14.3的化学键参数计算

使用复杂晶体上化学键理论计算了RBa2Cu4O8(R=Dy,Ho,Er,Tm,Yb)和Y2Ba4Cu7O14.3的化学键参数。结果表明,CuO1链上的CuO键共价性大于它们在CuO2面的共价性,当金属元素与氧形成五配位时,其共价性的数值大于这些元素在六配位时的情形。     

Eu2+在M3La3(BO3)4(M=Ca,Sr,Ba)中的发光性质

本文研究了Eu²⁺离子在M_yAl_xBO_y+3/2(1+x)(M=Ca,Sr,Ba)基质中的发光性质及磷和卤素对发光的影响。 采用以H₂和N₂混合气体为还原气氛在高温下进行固相反应的方法合成了一系列磷光体。发现,在CaAl_xBO_2.5+3/2x基质中,当X在0.5～2的范围内时及在Sr_yAl₂BO_{4 6+}基质中,当y在2～6的范围时掺入的Eu³⁺不能被H₂还原为Eu²⁺。其他Eu²⁺激活的磷光体一般都产生f～d跃迁的宽带发射,发射峰的波长随着基质组成的不同可在400～600nm的区间的变化。     

LaMsb2O7：R^3＋（M=Li,Na,K;R=Eu,Dy,Bi）的合成,组成,结构及发光性能

研究了激活离子Eu~(3 ),Dy~(3 )和Bi~(3 )在具有相同结构的LaMSb_2O_7(M=Li,Na,K)中的发光特性,得到了发白光的磷光体LaNaSb_2O_7:Dy~(3 )。讨论了化学键的共价程度对Eu~(3 )和Dy~(3 )超灵敏跃迁强度比的影响。发现当用281nm激发试样时,Bi~(3 )对Eu~(3 )具有敏化作用并解释了其原因。     

RE1—xBxF3—y（RE=Y,La,Ce,Gd;B=Ca,Ba）的敏感性质的研究

LaF_3作为离子选择性电极和对气体的敏感性质已进行了一定的研究,但其他稀土氟化物的敏感性质却未见报道。本文合成了RE_(1-x)B_xF_(3-y),研究了它们的结构、电学性质及敏感性质,得到有可能在150℃使用的固体电解质氧敏材料。 (一) RE_(1-x)B_xF_(3-y)的结构分析 结构分析表明,Ca、Ba置换RE的含量少时,如La_(0.95)Ba_(0.05)F_(3-y)、Ce_(0.95)Ca_(0.05)F_(3-y)的X射线衍射分析结果与LaF_3、CeF_3相似,说明它们是固溶体。而Ca置换RE含量较多时,如Y_(0.71)Ca_(0.29)F_(3-y)、Gd_(0.85)Ca_(0.15)F_(3-主)的X射线衍射分析结果却与相应的YF_3和GdF_3完全不     

Kathodolumineszenz der neuen Selten Erd-aktivierten Granate A2A′Sb2Zn3O12 (A = Gd,Y; A′ = Sr,Ca)

By activation of the new garnet host lattices A₂A′Sb₂Zn₃O₁₂ (A = Gd, Y; A′ = Sr, Ca) with the trivalent rare earth ions (Ln³⁺ = Pr, Eu, Tb, Tm) a cathodoluminescence in the visible region is observed. The influence of the electronic structure and concentration of the activator on the relative intensity as well as the host lattice participation in the energy transfer processes are discussed.     

Über die verbreitung ternärer komplexnitride mit Perowskitstruktur in SE-Al-N-systemen (SE ≡ La,Ce, Pr,Nd, Sm,Gd, Tb,Dy, Ho,Er, Tm,Yb, Lu)

The existence of complex nitrides in the RE-Al-N (RE ≡ rare earth) ternaries is investigated. In the systems containing lanthanum, cerium, praseodymium, neodymium and samarium either ternary phases (RE)₃AlN_x with a perovskite-type structure or alternatively almost complete filling of the octahedral voids by nitrogen in (RE)₃Al phases with an L1₂-type structure are found. An isothermal section for Pr-Al-N at 600 °C is presented. In the systems RE-A1-N (RE ≡ Gd, Tb, Dy, Ho, Er, Tm, Yb, Lu) no ternary phase is observed.     

A systematic study on the crystal structure and properties of RuSr2RCu2O8−δ (R=Gd,Tb, Dy,Y, Ho,Er)

The coexistence of superconductivity and magnetic order seems to take place in the so-called ruthenate-cuprates (Ru-1212). A systematic study is carried out on crystal structure of the RuSr₂RCu₂O_8−δ phases (R=Gd, Tb, Dy, Y, Ho, Er) synthesized under high pressure by X-ray powder diffraction. RuSr₂RCu₂O_8−δ (R=Gd, Tb, Dy, Y, Ho, Er) has the Ru-1212-type structure of a tetragonal symmetry and the RuO₆ octahedra rotate around the c-axis with an additional small rotation around an axis perpendicular to c. The DC-magnetization data establish that compounds with R=Gd, Y, Ho, Er exhibit ferromagnetic order below about 140 K, and the Meissner effect was observed at low temperature for R=Y compound.     

KCl-NaCl(1:1mol)-RECl_3熔体的电导率(RE=La、Ce、Pr、Nd、Sm、Eu、Gd、Tb、Dy、Ho、Er、Tm、Yb、Lu、Y、Ce族、Y族)

用交流电桥法测定了熔融KCl-NaCl(1:1摩尔)-RECl_3的电导。比电导的温度函数表达式如下: k=A+B(t-700) k:比电导(Ω~(-1)·cm~(-1));t:温度(700—850℃); A、B:本文给出的常数。 讨沦了实验值与计算值的偏差,当稀土氯化物在熔体中的浓度为10—50重量百分数时可能形成了络合物。     

KCl-NaCl(1:1mol)-RECl3熔体的电导率(RE=La、Ce、Pr、Nd、Sm、Eu、Gd、Tb、Dy、Ho、Er、Tm、Yb、Lu、Y、Ce族、Y族)

用交流电桥法测定了熔融KCl-NaCl(1:1摩尔)-RECl₃的电导。比电导的温度函数表达式如下: κ=A+B(t-700) κ:比电导(Ω^-1·cm^-1);t:温度(700—850℃); A、B:本文给出的常数。讨沦了实验值与计算值的偏差,当稀土氯化物在熔体中的浓度为10—50重量百分数时可能形成了络合物。     

Regularities of change in the structural parameters of EuLnCuS<Subscript>3</Subscript> (Ln = La–Nd,Sm, Gd,Ho)

Regularities of change in the structural parameters of EuLnCuS₃ (Ln = La–Nd, Sm, Gd, Ho) at an annealing temperature of 970 and 1170 K have been established. A decrease in the Ln³⁺ ionic radius results in the consecutive change of structural types (STs) for the compounds: α-EuLnCuS₃ (Ln = La, Ce, Pr, Nd; BaLaCuS₃ ST) → β-EuLnCuS₃ (Ln = Ce, Pr, Nd; Ba2MnS₃ ST) → γ-EuLnCuS₃ (Ln = Sm, Gd, Ho; Eu₂CuS₃ST). The change of structural types for EuLnCuS₃ leads to a jump-like change in their unit cell parameters and the transformation of coordination polyhedra shaped as a one-capped trigonal prism LnS₇ (α and β phases) into an octahedron LnS₆ (γ phases). The appearance of morphotropic changes correlates with the tetrad effect.     

(Li,Ca,A)_2SiO_4:Eu,Bi发光体的合成和发光性能的研究(A=Al,Y,La,Gd)

为了寻找新的发光基质材料,用高温固相反应合成了(Li,Ca,A)_2SiO_4:Eu,Bi系列发光体(A=Al,Y,La,Gd).通过激发光谱和发射光谱的测试.首次在碱土金属硅酸盐体系中研究了Al,Y,La,Gd等三价金属离子对Bi~(3+)、Eu~(3+)发光特性和Bi~(3+)敏化Eu~(3+)发光性能的影响,得到了良好的基质组成.实验结果表明.基质中适当含量的Gd~(3+)可大幅度提高Eu~(3+)的发光强度,使~5D_0-~7F_2发射强度增加6倍.Bi~(3+)对Eu~(3+)有很好的敏化作用,以A=Gd或Al时较好,对~5D_0-~7F_1辐射跃迁的敏化效果尤为突出.     

M2B5O9X∶Eu,Tb(M=Ca,Sr;X=Cl,Br)荧光体的光谱特征

利用Eu3+和Tb3+稀土离子之间存在电子组态共轭性的特征,将其双掺于同一基质中,由于电子转移而产生Eu2+,使Eu3+,Tb3+和Eu2+共存于同一体系中.在空气中合成了M2B5O9X∶Eu,Tb荧光粉,研究了其发光特征及影响作用.结果表明,Eu3+,Tb3+和Eu2+共存于同一基质中,且稀土离子的掺杂量对其光谱产生影响.     

La1—xMxFeyCo1—yO3型复合氧化物（M=Sr,Ba）的合成,结构及电性能

钙钛矿型的稀土与过渡金属复合氧化物(ABO_3)及部分稀土为碱土金属置换的A_(1-x)M_xBO_3型复合物在最近20年来研究较多,并在催化气敏,超导等方面取得了良好进展。但对A_(1-x)M_xB_(1-y)N_yO_3型复合物却研究甚少。本文合成了一系列的La_(1-x)M_xFe_yCo_(1-y)O_3(M=Sr或Ba)钙钛矿型复合氧化物,研究了它们组成与电性的变化规律。     

The phase diagram and tetragonal superstructures of the rare earth cobaltate phases Ln1−xSrxCoO3-δ (Ln=La, Pr, Nd, Sm, Gd, Y, Ho, Dy, Er, Tm and Yb)

Single phase perovskite-based rare earth cobaltates (Ln_1−xSr_xCoO_3−δ) (Ln=La³⁺, Pr³⁺, Nd³⁺, Sm³⁺, Gd³⁺, Dy³⁺, Y³⁺, Ho³⁺, Er³⁺, Tm³⁺ and Yb³⁺; 0.67?x?0.9) have been synthesized at 1100°C under 1 atmosphere of oxygen. X-ray diffraction of phases containing the larger rare earth ions La³⁺, Pr³⁺ and Nd³⁺ reveals simple cubic structures; however electron diffraction shows orientational twinning of a local, tetragonal (I4/mmm; a_p×a_p×2a_p) superstructure phase. Orientational twinning is also present for Ln_1−xSr_xCoO_3−δ compounds containing rare earth ions smaller than Nd³⁺. These compounds show a modulated intermediate parent with a tetragonal superstructure (I4/mmm; 2a_p×2a_p×4a_p). Thermogravimetric measurements have determined the overall oxygen content, and these phases show mixed valence (3⁺/4⁺) cobalt oxidation states with up to 50% Co(IV). X-ray diffraction data and Rietveld techniques have been used to refine the structures of each of these tetragonal superstructure phases (Ln=Sm³⁺-Yb³⁺). Coupled Ln/Sr and oxygen/vacancy ordering and associated structural relaxation are shown to be responsible for the observed superstructure.     

M2B5O9X：Eu，Tb（M=Ca,Sr;X=Cl,Br）荧光体的光谱特征

利用Eu^3 和Tb^3 稀土离子之间存在电子组态共轭性的特征,将其双掺于同一基质中,由于电子转移而产生Eu^2 ,使Eu^3 ,Tb^3 和Eu^2 共存于同一体系中,在空气中合成了M2B5O9X：Eu,Tb荧光粉,研究了其发光特征及影响作用。结果表明,Eu^3 ,Tb^3 和Eu^2 共存于同一基质中,且稀土离子的掺杂量对其光谱产生影响。     

Structural features of phases (Na<Subscript>0.5</Subscript>R<Subscript>0.5</Subscript>)MO<Subscript>4</Subscript> and (Na<Subscript>0.5</Subscript>R<Subscript>0.5</Subscript>)MO<Subscript>4</Subscript>:R′ (R = Gd,La; R′ = Er,Tm, Yb; M = W,Mo) of the scheelite family

The structural data for single crystals of (Na_0.5R_0.5)MO₄ and (Na_0.5R_0.5)MO₄:R′ (R = La, Gd; R′ = Er, Tm, Yb; M = W, Mo) grown by the Czochralski method were studied by X-ray diffraction and analyzed. The structural characteristics of these compounds depend on the sort of cations M and R. The formation of superstructures was found in the scheelite structure, and distortion of the scheelite structure depending on the composition and preparation conditions was established (with unit cell rotation by 45° and triclinic distortion of the scheelite structure for (Na_0.5Gd_0.5)WO₄:Tm, with doubled unit cell compared to the scheelite type structure for (Na_0.5Gd_0.5)WO₄ and (Na_0.5Gd_0.5)WO₄:Yb). In the case of overstoichiometric oxygen content in the crystal, the unit cell symmetry increases to space group I4₁/amd or (Na_0.5Gd_0.5)WO₄:Yb without considerable change in the cell parameters. On the basis of experimental data, a transformation scheme for the structures in the system Na ₂ ⁺ M⁶⁺O_4?-“R³⁺M⁵⁺O₄” was proposed.     

在空气中合成MBPO5:Eu2+和MBPO5:Yb2+(M=Ca,Sr,Ba)荧光体

以含RE₂O₃(RE=Eu, Yb)为起始物, 在空气中成功地合成了MBPO5:RE(²⁺)(M=Ca, Sr, Ba;RE(²⁺)=Eu(²⁺), Yb(²⁺))荧光体, 测定了它们的激发和发射光谱峰位以及发射半高宽.     

Syntheses, structure, and luminescent properties of novel hydrated rare earth borates Ln2B6O10OH4•H2O (Ln = Pr, Nd, Sm, Eu, Gd, Dy, Ho, and Y)

Ln(2)B(6)O(10)(OH)(4)?H(2)O (Ln = Pr, Nd, Sm-Gd, Dy, Ho, and Y), a new series of hydrated rare earth borates, have been synthesized under hydrothermal conditions. A single crystal of Nd analogue was used for the structure determination by X-ray diffraction. It crystallizes in the monoclinic space group C2/c with lattice constants a = 21.756(4), b = 4.3671(9), c = 12.192(2) ?, and β = 108.29(3)°. The other compounds are isostructural to Nd(2)B(6)O(10)(OH)(4)?H(2)O. The fundamental building block (FBB) of the polyborate anion in this structure is a three-membered ring [B(3)O(6)(OH)(2)](5-). The FBBs are connected by sharing oxygen atoms forming an infinite [B(3)O(5)(OH)(2)](3-) chain, and the chains are linked by hydrogen bonds, establishing a two-dimensional (2-D) [B(6)O(10)(OH)(4)?H(2)O](6-) layer. The 2-D borate layers are thus interconnected by Ln(3+) ions to form the complex three-dimensional structure. Ln(2)B(6)O(10)(OH)(4)?H(2)O dehydrates stepwise, giving rise to two new intermediate compounds Ln(2)B(6)O(10)(OH)(4) and Ln(2)B(6)O(11)(OH)(2). The investigation on the luminescent properties of Gd(2-2x)Eu(2x)B(6)O(10)(OH)(4)?H(2)O (x = 0.01-1.00) shows a high efficiency of Eu(3+) f-f transitions and the existence of the energy transfer process from Gd(3+) to Eu(3+). Eu(2)B(6)O(10)(OH)(4)?H(2)O and its two dehydrated products, Eu(2)B(6)O(10)(OH)(4) and Eu(2)B(6)O(11)(OH)(2), present the strongest emission peak at 620 nm ((5)D(0) → (7)F(2) transition), which may be potential red phosphors.