稀土配合物的发光特性及其能量传递研究

利用激光诱导荧光技术研究了稀土铕等金属配合物的发光特性及其能量传递动力学过程．得到了这些稀土配合物中中心离子Eu（3 ）的激发光谱，配体的三线态发时光谱和单线态发射光谱；在实验上观察到由于中心离子Eu（3 ）的5D2←7F0马跃迁吸收造成的配体发射光谱中的凹陷行为     

Eu(Ⅲ)离子光谱探针配合物Eu(DMBM)(TPPO)_2(NO_3)_2中Eu(Ⅲ)的格位

77K下测得的激光激发光谱和发光光谱表明,配合物Eu(DMBM)(TPPO)_2(NO_3)_2(DMBM:二对甲氧基苯甲酰甲烷;TPPO:三苯基氧化膦)中的Eu(Ⅲ)离子具有两种晶格格位。~5D_0→~7F_I(0～2)跃迁光谱说明这两种铕(Ⅲ)格位的点群对称性分别是C_(2v)和C_1(或C_2或C_5)。有较高对称性(C_(2v))的格位在配合物中占优势。     

三-(β-戊二酮)-1,10-邻菲绕啉合铕(Ⅲ)的电子结构和化学键

1,10-邻菲绕啉是一类重要的双齿含氮配体,能与许多过渡金属及镧系金属形成络合物。系统和深入地了解稀土与1,10-邻菲绕啉所形成的配合物性质、结构和成键规律,对稀土的研究和利用具有一定的意义。 Melby等制备了多种镧系络合物,并测定了散射光谱。络合物三-(β-戊二酮)-1,10-邻菲绕啉合铕(Ⅲ)[Eu(C_5H_7O_2)_3(C_(10)H_8N_2)]的荧光光谱存在着~5D_0→~7F_0、~5D_0→~7F_1和~5D_0→~7F_2三种可能的跃迁,从这种低对称性络合物的荧光光谱中不能确定它的分子结构。Watson等用单晶X射线衍射测定了该络合物的晶体结构属单斜晶系,空     

双核双配体稀土配合物Tb1-xEux(TTA)3Phen的合成及光学性能研究

合成了系列铕铽双核稀土有机稀土配合物Tb1-xEux（TTA）3Phen，通过差热．热重分析、XRD、红外光谱、紫外光谱和荧光光谱等测试手段研究了配合物的组成、结构和发光性质。由紫外可见光谱可以看出，稀土有机配合物的吸收峰主要来自有机配体HTrA和1，10-Phen；差热-热重分析证明，稀土有机配合物热稳定性较好。荧光光谱和电致发光表明，铽对铕配合物的发光有协同作用。在该系列配合物中，不仅有机配体可以将吸收的能量传递给发光的铕离子使其发光，而且铽离子也可将其吸收的能量通过分子内能量传递给铕离子，增强铕的发光强度。同时就双核稀土有机配合物光致发光和电致发光的特性及掺杂体系的能量传递过程进行了讨论。     

(Y,Gd)BO_3∶Eu的真空紫外光谱特性

近年来由于等离子体平板显示 (PDP)技术的需要 ,对真空紫外 (VUV)光激发的荧光粉的研究成为发光材料领域中的一个新方向 [1～ 3] .由于技术和实验仪器等方面的原因 [4 ] ,以往人们对稀土发光材料VUV区的研究很少 ,缺乏对其光谱和能级的完整认识 .另外 ,稀土离子 Gd3+在荧光粉的能量传递中具有特殊作用 ,一些含 Gd3+的发光材料在 VUV区发光效率很高 ,例如 ,(Y,Gd) BO3∶ Eu在 VUV区的发光效率比 YBO3∶ Eu提高了 2 0 % ,比 Y2 O3∶ Eu提高了 1 .8倍 ,与其它红粉相比更具有实际应用价值 [4 ,5] .但目前对于 (Y,Gd) BO3∶ Eu的研…     

稀土(Gd3+,La3+)对Eu(p-MOBA)3phen/PMMA荧光及温敏特性的影响

以稀土氧化物(Eu_2O_3,Gd_2O_3,La_2O_3)、对甲氧基苯甲酸(p-MOBA)、菲咯啉(phen)为原料制备了不同稀土离子(Gd~(3+),La~(3+))掺杂的Eu(p-MOBA)_3phen探针分子。将所合成的探针分子与甲基丙烯酸甲酯(MMA)混合,以过氧化苯甲酰(BPO)为引发剂引发聚合,制得不同稀土(Gd~(3+),La~(3+))掺杂的Eu(p-MOBA)_3phen/PMMA温敏漆样品。利用扫描电镜、紫外-可见吸收光谱、红外光谱和荧光光谱对探针分子的形貌、结构、发光性能及温敏漆的荧光温度猝灭特性进行表征。红外光谱、紫外可见吸收光谱及扫描电镜能谱分析表明,Eu~(3+)与配体p-MOBA、phen成功配位,且掺入的稀土离子(Gd~(3+),La~(3+))未改变Eu(p-MOBA)_3phen结构,说明掺入的稀土离子(Gd~(3+),La~(3+))部分取代了Eu~(3+)。荧光光谱表明,稀土离子(Gd~(3+),La~(3+))的掺入对Eu(p-MOBA)_3phen的发光均具有增益作用,并且相应的温敏漆在50～100℃温度范围内都具有良好的荧光温度猝灭特性。而且相比于镧掺杂的Eu(p-MOBA)_3phen/PMMA,钆掺杂的Eu(p-MOBA)_3phen/PMMA具有更强的荧光发射和更高的测温灵敏度。可见,不同的稀土(Gd~(3+),La~(3+))对Eu(p-MOBA)_3phen/PMMA的荧光及温敏特性影响是不同的。     

YTaO4：Gd,Eu体系光致发光中的能量传递

用高温固相反应法合成了钆、铕离子双掺杂的正钽酸盐化合物YTaO4 :Gd ,Eu ,研究了该体系在紫外光激发下的发光性能 .对该体系激发、发射及漫反射光谱的研究表明 ,Gd3 离子在发光过程中可以作为能量传递的中介 ,该体系在发光过程中存在钽酸根到Eu3 离子 ,或者钽酸根到Gd3 离子、再到Eu3 离子的能量传递     

Y2O3∶Eu3+发光薄膜的溶胶-凝胶法制备、表征及图案化

采用Pechini溶胶-凝胶法制备了纳米级Y2O3∶Eu3+发光薄膜, 同时, 通过软石印技术得到了条纹宽度为5～60 μm的Y2O3∶Eu3+图案化发光薄膜. 通过X射线衍射 (XRD)、付里叶变换-红外光谱 (FT-IR)、原子力显微镜(AFM), 光致发光(PL)光谱及寿命等方法对得到的发光薄膜进行了表征. XRD结果表明500 ℃时薄膜开始结晶, 900 ℃已结晶完全, 得到了立方相的产物. 图案化的条纹在烧结的过程中发生了明显的收缩(50%). Y2O3基质向掺杂的稀土离子Eu3+发生了有效的能量传递, 使得Eu3+显示出5D0-7FJ(J=0, 1, 2, 3, 4)特征发射. 寿命和光致发光光谱的研究表明, 发光强度随着温度的升高而增强.     

Tb~(3+)离子在镧、钇、钆二元硫氧化物固溶体中的发光研究

用稀土氧化物硫化法合成了发光体(La_(0.9)Gd_(0.1))_2O_2S:Tb,(La_(0.9)Y_(0.1))_2O_2S:Tb和(Y_(0.8)Gd_(0.2))_2O_2S:Tb,用X射线、阴极射线和254nm 紫外线三种激发方式测试了不同Tb~(3+)离子浓度(每摩尔基质中含0.0001～0.1摩尔Tb~(3+))时,它们的发光性能。测定了它们的发光亮度、发光色度随激活剂Tb~(3+)离子浓度的变化,研究了在这三种发光体中Tb~(3+)离子的~5D_3→~7F_J和~5D_4→~7F_J 的能级跃迁强度随Tb~(3+)离子浓度变化的关系。最后探讨了激活剂 Tb~(3+)离子在这三种发光体中的浓度猝灭机理。     

铕、铽2,6-二甲酸吡啶、α-甲酸吡啶络合物的研究

近年来,稀土络合物的发光引起了人们的重视。Yamazoe等报道了R-CH=CH-COO~-类及β-羧酸吡啶铕、铽络合物的发光性能。山添等报道了α-甲酸吡啶铕、铽络合物的摩擦发光。本文制备了铕和铽的2,6-二甲酸吡啶络合物Na_3[Ln(DPA)_3]·NaCl·_3H_2O和α-甲酸吡啶络合物Ln(DPA)(PA)·1.5NaCl·3H_2O(Ln=Eu、Tb;DPA=2,6-二甲酸吡啶酸根;PA=α-甲酸吡啶酸根),并测定了络合物的红外光谱和荧光光谱。     

Intercalation of organic sensitisers into layered europium hydroxide and enhanced luminescence property

Two organic sensitisers 4-biphenylcarboxylate (BPC) and terephthalate (TA) were intercalated into the gallery of layered europium hydroxide (LEuH). PL spectra tests indicated that BPC markedly enhanced the red luminescence of Eu(3+) due to efficient energy transfer between BPC and Eu(3+), forming a contrast to intercalated TA and the starting NO(3)(-) anions in the gallery. The energy level matching of the organic guests and Eu(3+) was also discussed to explain the energy transfer from sensitiser to Eu(3+).     

Luminescence behavior of Eu3+ doped LaF3 nanoparticles

Europium-doped LaF3 nanoparticles have been prepared by the ionic reaction in the ethanol at 60 degrees C. From the XRD pattern of nanoparticles and the emission spectra of Eu3+ ions, it has been concluded that the Eu3+ ions could easily substitute the La3+ sites and the solid solution La(1-x)Eu(x)F3 can be synthesized. Due to very low phonon energies of LaF3 matrix, the 5D1 emission of Eu3+ ions in La(1-x)Eu(x)F3 nanoparticles can be observed at room temperature when doping concentration of Eu3+ ions is lower than 30 mol%. The quenching process of 5D1 emission can be attributed to cross-relaxation. Since clusters of Eu3+ ions and resonance energy transfer only occurs within one particle due to the hindrance by the particle boundary, the concentration quenching resulted from resonance energy transfer between neighboring Eu3+ ions occurs at higher Eu3+ concentrations in the Eu3+ doped LaF3 nanoparticles.     

Tuning the triplet energy levels of pyrazolone ligands to match the 5D0 level of europium(III)

Three pyrazolone-based ligands, namely 1-phenyl-3-methyl-4-(1-naphthoyl)-5-pyrazolone (HL1), 1-phenyl-3-methyl-4-(4-dimethylaminobenzoyl)-5-pyrazolone (HL2), and 1-phenyl-3-methyl-4-(4-cyanobenzoyl)-5-pyrazolone (HL3), were synthesized by introducing electron-poor or electron-rich aryl substituents at the 4-position of the pyrazolone ring. Their corresponding europium complexes Eu(LX)3(H2O)2 and Eu(LX)3(TPPO)(H2O) (X = 1-3) were characterized by photophysical studies. The characteristic Eu(III) emission of these complexes with at most 9.2 x 10(-3) of fluorescent quantum yield was observed at room temperature. The results show that the modification of ligands tunes the triplet energy levels of three pyrazolone-based ligands to match the 5D0 energy level of Eu3+ properly and improves the energy transfer efficiency from antenna to Eu3+, therefore enhancing the Eu(III) emission intensity. The highest energy transfer efficiency and probability of lanthanide emission of Eu(L1)3(H2O)2 are 35.1% and 2.6%, respectively, which opens up broad prospects for improving luminescent properties of Eu(III) complexes by the modification of ligands. Furthermore, the electroluminescent properties of Eu(L1)3(TPPO)(H2O) were also investigated.     

YTaO4：Gd,Eu体系光致发光中的能量传递

Yttrium orthotantalate co doped by Eu 3+ and Gd 3+ has been synthesized by solid state method. The emission and excitation spectra of YTaO4: Gd, Eu are studied in detail. In the excitation spectra of Eu 3+5D 0→ 7F2 transition emission in YTaO4:Gd, Eu, there appear excitations of Gd3+ and TaO43- group, which indicate energy transfer from Gd 3+ and TaO4 3- group to Eu 3+ in the process of luminescence. The excitation spectra of Gd 3+ emission(λ=312 5 nm) including strong excitation of charge transfer of group show energy transfer from host lattice to Gd 3+ . So there are two ways of energy transfer in YTaO4:Gd,Eu system. The strong evidences from excitation spectra, emission spectra and diffusive reflection spectra of this system show that Gd 3+ can play an intermediate role in the process of luminescence. There is energy transfer from TaO 3- 4 to Gd 3+ and finally to Eu 3+ via the charge transfer state and spectral overlap. The energy transfer from TaO 3- 4 to Gd 3+ is a dominating process in this system.     

Eu3+,Tb3+混配配合物的激光诱导荧光

利用激光诱导荧光技术研究了两种三价稀土金属离子的β－二酮与有机配体混配络合物中金属离子的寿命及其能级结构，得到了Ｅｕ＾３＋的能级常数。     

Fluorescence properties of Eu3+ ions doped borate and fluoroborate glasses containing lithium, zinc and lead

The influence of glass composition on the fluorescence properties of Eu3+ ions doped borate and fluoroborate glasses modified with Li+, Zn2+ and Pb2+ cations have been investigated. The magnitude of splittings of 7F1 levels are analyzed using crystal-field (CF) analysis. The relative intensities of 5D0 --> 7F2 to 5D0 --> 7F1 transitions, crystal-field strength parameters and decay times of the 5D0 level have been determined and are found to be lower for Pb based glasses than those of Zn/Li based glasses. The lifetimes of 5D0 level are found to increase when borate glasses are modified with pure fluorides than with oxides and oxyfluorides. The fluorescence decay of 5D0 level fits perfect single exponential in the Eu3+:glass systems studied which indicates the absence of energy transfer between Eu3+ ions in these glasses.     

Dependence of the Lifetime upon the Excitation Energy and Intramolecular Energy Transfer Rates: The (5) D(0) Eu(III) Emission Case

In many Eu(III) -based materials, the presence of an intermediate energy level, such as ligand-to-metal charge transfer (LMCT) states or defects, that mediates the energy transfer mechanisms can strongly affect the lifetime of the (5) D(0) state, mainly at near-resonance (large transfer rates). We present results for the dependence of the (5) D(0) lifetime on the excitation wavelength for a wide class of Eu(III) -based compounds: ionic salts, polyoxometalates (POMs), core/shell inorganic nanoparticles (NPs) and nanotubes, coordination polymers, β-diketonate complexes, organic-inorganic hybrids, macro-mesocellular foams, functionalized mesoporous silica, and layered double hydroxides (LDHs). This yet unexplained behavior is successfully modelled by a coupled set of rate equations with seven states, in which the wavelength dependence is simulated by varying the intramolecular energy transfer rates. In addition, the simulations of the rate equations for four- and three-level systems show a strong dependence of the emission lifetime upon the excitation wavelength if near-resonant non-radiative energy transfer processes are present, indicating that the proposed scheme can be generalized to other trivalent lanthanide ions, as observed for Tb(III) /Ce(III) . Finally, the proper use of lifetime definition in the presence of energy transfer is emphasized.     

GdF3∶Eu3+/NaGdF4∶Eu3+纳米晶的水热合成及发光性质

采用水热法,以聚乙二醇(400)为分散剂,以NaOH和HNO3溶液调节初始溶液pH值,合成GdF3∶Eu3+和NaGdF4∶Eu3+纳米晶。XRD和SEM结果表明:在酸性溶液(pH=3,5)、中性溶液(pH=7)和碱性溶液(pH=9)中,分别获得具有正交结构的GdF3∶Eu3+纳米晶,GdF3∶Eu3+和NaGdF4∶Eu3+混合晶,六方结构NaGdF4∶Eu3+棒状微米晶。根据Scherrer公式估算pH=3和pH=5时制备纳米晶的一次性粒径分别为49和28 nm。样品的发射光谱结果表明:特征发射峰来自于5D2、5D1、5D0到7FJ跃迁。在主晶相为GdF3样品中,主发射峰来自于Eu3+的5D0→7F1的磁偶极跃迁;晶相为NaGdF4样品的主发射峰来自于Eu3+的5D0→7F2电偶极跃迁。5D0→7F1和5D0→7F2跃迁发射相对强度比值显示:Eu3+在NaGdF4晶体中的格位对称性下降。激发光谱显示出Gd3+和Eu3+具有较好的能量传递。     

Ce3+,Tb3+,Eu3+共掺杂Sr2MgSi2O7体系的白色发光和能量传递机理

通过正交试验,采用高温固相法制备了Sr2-x-y-zMgSi2O7∶xCe3+,yTb3+,zEu3+系列样品.使用X射线衍射仪和荧光光谱仪表征了样品的物相和发光性质,并讨论了Ce3+-Tb3+-Eu3+共掺杂Sr2MgSi2O7体系中的能量传递过程.实验结果表明,在327 nm波长激发下,所合成荧光粉的发射峰主要位于387 nm(蓝紫)、542nm(绿)和611 nm(红)处;分别以387,542和611 nm为监控波长,所得激发光谱显示荧光粉在327 nm处有最好的激发.在327 nm光激发下,系列样品发光进入白光区.最优化的荧光粉为Sr1.91MgSi2O7∶0.01Ce3+,0.05Tb3+,0.03Eu3+,其色坐标为(0.337,0.313),是一种潜在的发光二极管(LED)用白色荧光粉.     

3-Phenyl-4-benzoyl-5-isoxazolonate complex of Eu3+ with tri-n-octylphosphine oxide as a promising light-conversion molecular device

Three new europium complexes, [Eu(PBI)3.3H2O] (1), [Eu(PBI)3.2TOPO] (2), and [Eu(PBI)3.2TPPO.H2O] (3) (where HPBI, TOPO, and TPPO stand for 3-phenyl-4-benzoyl-5-isoxazolone, tri-n-octylphosphine oxide, and triphenylphosphine oxide, respectively), with different neutral ligands were synthesized and characterized by elemental analysis, Fourier transform infrared, (1)H NMR, thermogravimetric analysis, and photoluminescence (PL) spectroscopy. The coordination geometries of the complexes were calculated using the Sparkle/AM1 (Sparkle Model for the Calculation of Lanthanide Complexes within the Austin Model 1) model. The ligand-Eu3+ energy-transfer rates were calculated in terms of a model of the intramolecular energy-transfer process in lanthanide coordination compounds reported in the literature. The room-temperature PL spectra of the europium(III) complexes are composed of the typical Eu3+ red emission, assigned to transitions between the first excited state (5D0) and the multiplet (7F(0-4)). On the basis of emission spectra and lifetimes of the 5D0-emitting level, the emission quantum efficiency (eta) was determined. The results clearly show that the substitution of water molecules by TOPO leads to greatly enhanced quantum efficiency (i.e., 26% vs 92%) and longer 5D0 lifetimes (250 vs 1160 micros). This can be ascribed to a more efficient ligand-to-metal energy transfer and a less nonradiative 5D0 relaxation process. Judd-Ofelt intensity parameters (Omega2 and Omega4) were determined from the emission spectra for the Eu3+ ion based on the 5D0 --> 7F2 and 5D0 --> 7F4 electronic transitions, respectively, and the 5D0 --> 7F1 magnetic-dipole-allowed transition was taken as the reference. A point to be noted in these results is the relatively high value of the Omega2 intensity parameter for all of the complexes. This may be interpreted as being a consequence of the hypersensitive behavior of the 5D0 --> 7F2 transition. The dynamic coupling mechanism is, therefore, dominant, indicating that the Eu3+ ion is in a highly polarizable chemical environment.