(Y,Gd)Al3(BO3)4∶Ce,Tb的光谱特性及稀土离子间的能量传递

采用高温固相反应合成了(Y,Gd)Al3(BO3)4中掺杂Ce3 和Tb3 的样品,并研究了其结构特性、光谱特性和发光过程中稀土离子间的能量传递.(Y,Gd)Al3(BO3)4属于三角晶系,具有R32的空间群,掺入Ce3 ,Tb3 杂质后晶格结构没有变化.(Y,Gd)Al3(BO3)4∶Ce,Tb的激发光谱由3个宽谱带组成,这3个谱带分别对应于Ce3 的4f-5d跃迁吸收.在该体系中存在Ce3 →Tb3 ,Gd 3 →Tb3 和Gd3 →Ce3 的能量传递,其中Ce3 起敏化剂和中间体的双重作用.     

偏硼酸钆镁:铈(Ⅲ)、铽(Ⅲ)、锰(Ⅱ)高显色性荧光粉的研制

用高温固相反应法合成了高显色性橙红粉(Gd，Ce，Tb)(Mg，Mn)B5O10，研究了硼酸用量、Tb／Ce比例、氢气浓度和灼烧温度等对合成产物发光性能的影响。实验表明，当硼酸过量8％、Tb／Ce≥2．5、氢气浓度≤10％、灼烧温度≥1000℃时，可制得发光亮度较高的高显色性橙红色荧光粉。为进一步探讨Tb，Mn的激活机制，制备了高显色性绿粉(Gd，Ce，Tb)MgB5O10和高显色性红粉(Gd，Ce)(Mg，Mn)B5O10作对比。研究表明，通过无辐射能量机制，Ce^3 能够有效地将吸收的紫外能量传递给Tb^3 ，Gd^3 作为能量传递过程中的中间体，其作用是增强Tb^3 的发光，即发生了“激发→Ce^3 →(Gd^3 )n→Tb^3 →发射”过程。此外，Mn^2 发光不能被Ce^3 直接敏化，也是通过Gd^3 作为中间体，发生Gd^3 →Mn^2 的能量传递。     

Dy^3＋在Ba3La（B03）3中的光致发光

研究了Ba3La(BO3)3基质中Dy^3 的光致发光特性；探讨了RE^3 的电荷半径比(z／r)和Ce^3 ，Dy^3 含量对Dy^3 发光强度及发光颜色的影响；分析了Ba3La(BO3)3中Ce^3 对Dy^3 发光的敏化作用；确定了Dy^3 的^4F9／2→^6H15／2及^4F9／2→^6H13/2跃迁发射的浓度猝灭机制均为电偶极-电四极相互作用。     

Synthesis and Structure of Ba3La2（BO3）4 Crystal

1 INTRODUCTION At present the researches on more efficient solid-state laser materials become more important for the rapid development of diode-laser pumped solid-state laser. More researches have been devoted to the double borate compounds RX3(BO3)4 (R = Y, La, Gd and X = Y, Al, Sc), some of which exhibit good chemical and physical properties[1～10]. The rare earth and alkali-halide double borates M3Ln2(BO3)4 (M = Ca, Sr, Ba and Ln = LaLu and Y) were reported in literatures[11…     

LaAl3(BO3)4的合成及其晶体结构的研究

在研究LnAl3(BO3)(Ln=稀土元素，Y）的合成及发光特性过程中，发现镧铝硼酸盐LaAl3(BO3)4具有一种新的晶体结构。本文用助熔剂法合成了LnAl3(BO3)4(Ln=Gd,La)单晶样品，LaAl3(BO3)4为薄板状，而GdAl3(BO3)4为六方的棒状，用TREOR90程序对LaAl3(BO3)4粉末样品的X射线衍射数据进行了指标化，结果为：LaAl3(BO3)4属正交晶系，晶胞参数为a=0.93586(4)nm,b=0.79904(3)nm,c=0.40626(6)nm,V=0.34595nm^3，在1000℃空气环境下，用硝酸盐热分解法合成了单相LnAl3(BO3)4:E3 （Ln=Gd,La)荧光粉并研究了其发光特性，结果表明：LnAl3(BO3)4:Eu^3 (Ln=Gd,La)是非常有前途的等离子显示器用荧光粉。     

Zn4B6O13∶ Ce3+, Tb3+ 的合成与发光

高温固相扩散方法首次合成了Zn4B6O13:Ce^3 ,Tb^3 光致光材料。通过XRD分析获得晶胞参数：α=0.7472nm,V=0.4172nm^3,为立方晶系，研究Ce^3 和Ce^3 ,Tb^3 在Zm4B6O13中的激发和发射光谱，发现Ce^3 在Zn4B6O13中的激发和发射带比Ce^3 在其他基质中红移2.38-4.94KK,Ce^3 的发射带与Tb^3 与^7F6→^5G2,^5D1,^5H7吸收带有很好的重叠，使Ce^3 对Tb^3 有良好的敏化作用。Ce^3 ,Tb^3 在基质中的能量传递机理为：Ce^3 →Ce^3 和Ce^3 →Tb^3 之间的偶极子－－偶极子的电多级相互作用的共振传递机理，色坐标为：x=0.281,y=0.619。SEM摄取产物晶貌，颗粒均匀，平均粒度为0.23μm，接近纳米级。     

Crystal Structure of Lithium Yttrium Borate LiY6O5（BO3）3

1 INTRODUCTION In recent years, more and more attention has been paid to rare-earth borates due to their excellent pro- perties, such as YCa4O(BO3)3(YCOB)[1], YAl3(BO3)4 (YAB)[2] and La2CaB10O19[3] for nonlinear optical materials and self-frequency doubling materials as well as YBO3:Eu for red phosphor materials[4] and Li6M1-xCex(BO3)3 (M = Y, Gd) for neutron detec- tors[5]. In this work, we focus our research interest on LiY6O5(BO3)3 as hosts for VUV (vacuum ultraviolet) l…     

Ca_4GdO(BO_3)_3:Eu~(3 ),Sm~(3 )的发光及离子间的能量转移

Ca4 RO( BO3 ) 3 ( R=La,Ln,Y)三硼酸盐具有优良的非线性特征 . Khamaganova等[1] 以Pb O作助熔剂在合成 Ca4 Sm2 ( BO3 ) 4的过程中发现了一种新相 ,经过结构分析判定是一种新的化合物 .Norrestam等通过高温固相反应合成出此类三硼酸盐 .Iiykhuin[2 ] 对 Ca4 RO( BO3 ) 3( R=Lu,Tb,Gd)的结构进行了研究 .Dirkse等 [3 ]报道了 Ca4 Gd O( BO3 ) 3 粉末的发光特性 .1 996年 ,Aka[4 ] 采用提拉法 ( Czochralski)首次生长出较大尺寸的 Ca4 Gd O( BO3 ) 3 单晶 .孟宪林等 [5]报道了 Ca4 YO( BO3 ) 3 :Nd晶体的激光发射和自倍…     

白光LED用荧光材料Ba3Gd（BO3）3∶Eu^（3＋）的发光性能研究

用高温固相反应法制备了稀土离子Eu^3＋掺杂的三元稀土硼酸盐Ba3Gd（BO3）3发光材料,通过X射线衍射（XRD）、荧光光谱和扫描电镜（SEM）等测试手段对Ba3Gd（BO3）3∶Eu^3＋荧光粉的制备条件、发光性能以及形貌进行了研究。XRD结果表明,在1000℃时可得到Ba3Gd（BO3）3纯相。扫描电镜照片显示颗粒基本为球形,粒径约为200-400 nm。发光光谱测试表明,Ba3Gd（BO3）3∶Eu^3＋荧光粉在近紫外区（UV）（396 nm）和蓝光区（466 nm）可以被有效地激发,分别用255和396 nm的紫外光激发样品时,以Eu3＋的5D0-7F2（611和616 nm）超灵敏跃迁为主要发射峰。当Eu3＋的掺杂浓度为10%（摩尔分数）时,Ba3Gd（BO3）3∶Eu3＋在611和616 nm处的发光强度最大。因此,这种荧光粉是一种可能应用在白光LED上的红色荧光材料。     

(Y,Gd)VO_4∶Eu~(3+)的紫外-真空紫外发光特性

用高温固相法合成了Y1-xGdxVO4∶Eu3 (0≤x≤1)系列单相样品并研究了其发光特性。在254nm激发下,观察到最大强度位于619nm的红色发射峰且其强度在Y/Gd=0.4/0.6时达到最大。在147nm激发下的发射峰与紫外下的一致,发射强度也是在Y/Gd=0.4/0.6时达到最大,大约是商用(Y,Gd)BO3∶Eu3 荧光体的65%。619nm监控下的真空紫外激发光谱由峰值位于158nm,204nm,247nm以及300nm的系列激发带组成,归属于钒酸根的基质吸收以及Gd3 、Y3 和Eu3 的电荷迁移带吸收。相对(Y,Gd)BO3∶Eu3 中Eu3 占据中心对称格位,(Y,Gd)VO4∶Eu3 中Eu3 占据非中心对称格位,其真空紫外下光谱色纯度更好。色坐标分别为(0.632,0.355),(0.672,0.328)。     

取代基对3(5)-(9-蒽基)吡唑光学性质的影响

使用密度泛函理论(DFT)B3LYP/6-31G(d)方法优化得到了3(5)-(9-蒽基)吡唑及其衍生物的基态(S₀)分子结构, 使用单激发组态相互作用(CIS)/6-31G(d)方法优化得到这些分子的第一单重激发态(S₁)的几何结构, 并使用含时密度泛函理论(TD-DFT)B3LYP/6-311++G(d,p)方法计算了它们的吸收和发射光谱. 计算结果表明, 与3(5)-(9-蒽基)吡唑相比, 无论取代基是吸电子基团还是供电子基团, 衍生物的吸收和发射峰均发生红移, 并且当取代基―R=―BH₂, ―CCl₃, ―CHO, ―NH₂时衍生物有较长的吸收波长和发射波长.     

Etude du Systeme LiPO3-Pr(PO3)3 Donnees sur LiPr(PO3)4

The LiPO₃-Pr(PO₃)₃ system was studied by micro-differential thermal analysis. The only new compound observed in the system was LiPr(PO₃)₄, melting incongruently at 1246 K. An eutectic appears at 926 K. Crystallographic data and powder diagram of the new compound are given. LiPr(PO₃)₄ crystallizes in the C2/c monoclinic system with unit cell: a=16.428(6), b=7.054(3), c=9.747(4) Å, β=126°31′(3), V=910.2 ų, Z=4. The IR and Raman spectra of this compound are given. This revised version was published online in July 2006 with corrections to the Cover Date.     

中性配合物Cr(acac)_3、mer-和fac-[Cr(bza)_3]的光学拆分

本文用新方法合成了Cr(bza)_3,改进了其mer-、fac-异构体的分离方法;增大了Cr(acac)_3的化学拆分量(1.5g)。试制了DBT(二苯甲酰-d-酒石酸)吸附型手性固定相(CSP),并成功地用于色谱拆分标题配合物的对映体,mer-[Cr(bza)_3]的部分拆分是首次发现的,其他配合物的拆分结果均优于文献方法。根据mer-[Cr(bza)_3)拆分流出液前、后组分的CD光谱,指定了其对映体绝对构型。还讨论了DBT吸附型CSP的拆分效能和色谱特性。     

中间体C60(CH3)-和产物C60(CH3)2的结构及产物

用INDO系列方法对C₆₀^2-与CH₃反应的中间体C₆₀(CH₃)^-进行理论研究,得到具有Cs对称性的构型。结果表明,CH₃加成到C₁₅上,将使与其相邻的双键碳(C₃₀)的电荷密度和自旋密度达极大值,故加成反应部位在C₃₀处;另外,C₁₅的对位C₁₂(或C₂₇)也较其它部位易于反应,且有两个反应场所,因而产物C₆₀(CH₃)₂可能为六元环上的1,2-加成和1,4-加成两种异构体的混合物。同时对两种加成产物的结构和电子光谱进行了理论研究,指认其电子跃迁,并讨论了其光谱红移的原因。     

3-(2-Quinolyl)- and 3-(5-carbethoxyfuryl-2)coumarins

3-(2-Quinolyl)- and 3-(5-carbethoxyfuryl-2)coumarins were prepared by reaction of substituted salicylaldehydes and hetarylacetonitriles. Alkylation and acylation of 3-hetaryl-7-hydroxycoumarins were studied. __________ Translated from Khimiya Prirodnykh Soedinenii, No. 5, pp. 432–434, September–October, 2005.     

Spectroscopy and Energy Transfer in Yb3＋ and Tm3＋ Co-doped Gd3Ga5O12 Crystal

Yb3+/Tm3+ co-doped Gd3Ga5O12 single crystal with a dimension of Φ30mm×20mm was grown successfully by Czochralski method.The absorption spectrum was recorded at room temperature and used to calculate the absorption cross-section.Based on the Judd-Ofelt(J-O) theory,we obtained the three intensity parameters and spectral parameters of this crystal,such as the line strengths,oscillator strengths,radiative probabilities and radiative lifetimes as well as the fluorescent branching ratios.Room temperature fluorescence spectra and luminescence decay curves were recorded.The energy transfer between Yb3+-Tm3+ was observed and the mechanism was discussed.The stimulated emission cross-section of the 3F4→3H6 transition was calculated by the Füchtbauer-Ladenburg(F-L) equation.The potential laser gains for this transition were also investigated.This crystal is promising as a tunable infrared laser crystal at 2.0 μm.     

Synthesis,crystal structure,and catalytic properties of a copper(I) complex with 3H-(1,2,3)triazolo(4,5-b)pyridin-3-ol

[Cu(tpol)]_n based on the Htpol ligand [Htpol = 3H-(1,2,3)triazolo(4,5-b)pyridin-3-ol] had been synthesized and characterized using X-ray single crystal analysis, elemental analysis, powder X-ray diffraction and IR spectroscopy. Catalytic activity of [Cu(tpol)]_n was measured by the coupling reaction of trifluoroacetimidoyl chlorides with terminal alkyne. The crystal shows two different coordination types of [tpol]^? having a parallelogram of [Cu₂O₂] assembled in a trans geometry. With the change of functional groups of two types of reactants, [Cu(tpol)]_n can replace the noble catalysts and selectively catalyze the coupling of derivatives of 2,2,2-trifluoro-N-phenylacetimidoyl chloride and terminal alkynes, and 6-methoxy-2-(trifluoromethyl)quinoline.