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1.
The positions of 15 electronic energy levels above the ground level 8S7/2 of Gd3+ in flux-grown single crystals of LiGdP4O12 have been determined from 4f–4f transitions observed in absorption spectra in the range 190–340 nm at T = 293 K. The experimental energy levels have been compared with theoretical ones obtained by two parameters, F2 = 392 cm−1 and ζ4f = 1525 cm−1, in the intermediate coupling approximation.  相似文献   

2.
Ping SuWen-Chen Zheng 《Optik》2012,123(22):2025-2027
The crystal field energy levels of laser crystal Gd3Ga5O12: Nd3+ are calculated using the diagonalization (of energy matrix) method. From the calculations, the 93 observed crystal field energy levels are explained reasonably and the root-mean-square (r.m.s.) deviation σ(≈25.6 cm−1) and the scalar crystal-field strength parameter Nv (≈3847 cm−1) are obtained. The results are discussed.  相似文献   

3.
Nanostructured samples of yttrium iron garnet Y3Fe5O12 obtained by plastic deformation method (high-pressure torsion) were studied with help of soft X-ray absorption spectroscopy using Fe 2p and O 1s spectra. Experimental spectra were compared with crystal field multiplet calculations for Fe ions. Some amount of Fe2+ ions in nanostructured Y3Fe5O12 was found. The concentration of Fe2+ ions was found to be increased with the increase of the degree of plastic deformation.  相似文献   

4.
Detailed analyses of spectroscopic and temperature-dependent magnetic susceptibility data are reported for the crystal-field split energy levels of the 7FJ and 5D4 of Tb3+ in stoichiometric single crystals of ortho-aluminate TbAlO3. The spectroscopic data include absorption spectra obtained between 2940 and 480 nm from 8 to 300 K. High resolution fluorescence spectra are reported, representing transitions from 5D4 to 7F6,5,4, at a sample temperature of 85 K. Using crystal-field modeling techniques recently adapted for low symmetry systems, we have assigned all 58 experimental Stark levels within the 7FJ and 5D4 manifolds, with a fitting standard deviation of 4.5 cm−1 (3.8 cm−1 rms error). As a further test, the theoretical Stark levels and calculated wavefunctions were used to determine the temperature dependence of the magnetic susceptibility along the c-axis of the TbAlO3 crystal. Good agreement is obtained between the calculated susceptibility and temperature-dependent magnetic data reported earlier, including a prediction of a 0.2 cm−1 splitting of the ground-state quasi-doublet. The susceptibility calculation also confirms the predicted ordering of states within the 7F6 multiplet manifold.  相似文献   

5.
用提拉法生长了掺铬、钕的钆镓石榴石(Cr4+,Nd3+∶GGG)自调Q激光晶体。报道了室温下的吸收光谱和荧光光谱特性。分析了Cr离子浓度对光谱性质的影响。比较了Cr4+∶GGG,Nd3+∶GGG和(Cr4+,Nd3+)∶GGG晶体吸收光谱的关系。测量了(Cr4+,Nd3+)∶GGG晶体和Nd3+∶GGG晶体的荧光寿命,它们分别是33μs和250μs。实验表明,(Cr4+,Nd3+)∶GGG晶体是一种非常有潜力的自调Q激光晶体,可以实现大功率激光器的小型化和全固态化。  相似文献   

6.
The paper is devoted to investigation of the processes of excitation energy transfer between the host cations (Tb3+ ions) and the activators (Ce3+ and Eu3+ ions) in single-crystalline films of Tb3Al5O12:Ce,Eu (TbAG:Ce,Eu) garnet which is considered as a promising luminescent material for the conversion of LED's radiation. The cascade process of excitation energy transfer is shown to be realized in TbAG:Ce,Eu: (i) from Tb3+ ions to Ce3+ and Eu3+ ions; (ii) from Ce3+ ions to Eu3+ ions by means of dipole-dipole interaction and through Tb3+ ion sublattice.  相似文献   

7.
利用X射线粉末衍射确定了Tm3+掺杂硅酸镓镧(La3Ga5SiO14,LGS)晶体的晶体结构;运用DICVOL91程序计算了该晶体不同部位的晶胞参数;测定了Tm:LGS晶体的室温吸收谱和470nm光激发下的发射光谱;根据Judd-Ofelt理论拟合了Tm3+的三个晶场调节参数Ωt(t=2,4,6),分别为2.694×10-20cm2,1.842×10-20cm2,0.030×10-20cm2;计算了各个能级跃迁的谱线强度、振子强度、吸收截面等,进而计算了3H43F4态的自发跃迁概率、辐射寿命、荧光分支比和积分发射截面,并对结果进行了分析. 关键词: Tm:LGS晶体 吸收谱 Judd-Ofelt理论 光谱参数  相似文献   

8.
Seven crystal field energy levels (obtained from the optical spectra) and three g factors gx, gy and gz (obtained from electron paramagnetic resonance (EPR) spectra) for Ce3+ ion in Y3Ga5O12 crystal are calculated together by diagonalizing a complete energy matrix. The Hamiltonian of this energy matrix includes all the interactions for 4f1 ion Ce3+ in rhombic crystal field and under an external magnetic field, and so the optical and EPR data can be studied in a unified way. The calculated crystal field energy levels are in better agreement with the experimental values than the calculated values in the previous paper, and the g factors (which have not been calculated previously) are explained reasonably. The results are discussed.  相似文献   

9.
The electronic structure of the Tm3+ in YAl3(BO3)4 crystals has been investigated by means of low temperature absorption and emission spectroscopy in the 5000-30,000 cm−1 range. The assignment of the lines composing the observed manifolds to transitions between the Stark levels of Tm3+ is complicated by the presence of extra features having different origins. The energy levels scheme of the doping ion has been compiled after a careful analysis of the spectra by reproducing the observed transitions by means of theoretical calculations based on a Hamiltonian, including the free ion and the crystal field (CF) terms. The agreement between experimental and calculated energy values was reasonably good, the overall r.m.s. deviation being 16 cm−1. The resulting CF parameters have been tabulated and compared with those reported in literature for other rare earth ions doped in YAB. The analysis of trends observed along the lanthanide series evidences some inconsistencies and the necessity of a systematic investigation of these systems.  相似文献   

10.
Binary (ZnO)0.5(P2O5)0.5 glasses doped with Eu2O3 and nanoparticles of Gd2O3:Eu were prepared by conventional melt-quench method and their luminescence properties were compared. Undoped (ZnO)0.5(P2O5)0.5 glass is characterized by a luminescent defect centre (similar to L-centre present in Na2O-SiO2 glasses) with emission around 324 nm and having an excited state lifetime of 18 ns. Such defect centres can transfer the energy to Eu3+ ions leading to improved Eu3+ luminescence from such glasses. Based on the decay curves corresponding to the 5D0 level of Eu3+ ions in both Gd2O3:Eu nanoparticles incorporated as well as Eu2O3 incorporated glasses, a significant clustering of Eu3+ ions taking place with the latter sample is confirmed. From the lifetime studies of the excited state of L-centre emission from (ZnO)0.5(P2O5)0.5 glass doped with Gd2O3:Eu nanoparticles, it is established that there exists weak energy transfer from L-centres to Eu3+ ions. Poor energy transfer from the defect centres to Eu3+ ions in Gd2O3:Eu nanoparticles doped (ZnO)0.5(P2O5)0.5 glass has been attributed to effective shielding of Eu3+ ions from the luminescence centre by Gd-O-P type of linkages, leading to an increased distance between luminescent centre and Eu3+ ions.  相似文献   

11.
12.
新型闪烁晶体Gd3(Al,Ga)5O12:Ce(GAGG:Ce)在制备过程中易出现包裹体及反格位缺陷等问题,严重影响晶体的性能.为了抑制这些缺陷以得到大尺寸高质量的GAGG:Ce晶体,本文以Gd3(Al,Ga)5O12为基质、Ce3+为掺杂离子,采用提拉法生长得到了GAGG:Ce晶体,并对不同晶体部位的物相结构、微区成分、透光性质、发光及时间性能进行了测试和对比分析.结果表明,GAGG:Ce晶体的透过谱中存在340和440 nm两处Ce3+特征吸收带,且位于550 nm处的直线透过率为82%.晶体尾部因杂相包裹体等宏观缺陷的影响,导致其透过率下降至70%左右.微区成分分析进一步表明GAGG:Ce晶体中存在三种类型的包裹体,分别为富Gd相、富Ce相及(Al,Ga)2O3相.GAGG:Ce晶体的X射线激发发射谱中在550 nm附近存在Ce3+宽发射带,且380 nm处还存在GdAl/Ga反格位缺陷引起的发射.晶体中存在的杂相包裹体及GdAl/Ga反格位缺陷等因素导致Ce3+在GAGG基质的发光强度下降12.5%;GdAl/Ga反格位离子与近邻Ce的隧穿效应使得GAGG:Ce晶体的衰减时间由117.7 ns延长至121.9 ns,且慢分量比例由16%增加至17.2%.  相似文献   

13.
A comparative study concerning the electronic structure of the Mn5+ ion in the Li3PO4, Ca2PO4Cl, Sr5(PO4)3Cl host lattices has been carried out in the framework of the exchange charge model. The crystal field parameters have been evaluated using the structural data as the only input information. The 10 K absorption spectra of the investigated compounds have been measured in order to verify the correspondence between experimental and calculated energy levels. A systematic trend of the crystal field splitting of the most intense transitions has been evidenced and discussed by considering the symmetry properties of the coordination polyhedra around Mn5+.  相似文献   

14.
The temperature dependence of the experimental results of dc (macroscopic) magnetic susceptibility and nuclear hyperfine properties of frustrated magnetic Gd-based pyrochlore compounds, Gd2Ti2O7, Gd2Sn2O7, Gd2Hf2O7 and Gd2Zr2O7, are analyzed within the frame work of appropriate crystal-field theory and a mean field approximation by introducing effective anisotropic molecular field tensors, and formulating an exact relation between single-ion susceptibility tensors and site susceptibility tensors. Components of the calculated susceptibility along and perpendicular to the local 〈1 1 1〉 axis of the tetrahedral sublattice of pyrochlore structure show that these pyrochlores are easy-planar anisotropic magnetic systems. The crystal-field parameters and anisotropic exchange coupling have been determined and their systematic variations over the Gd-based pyrochlores studied here are discussed.  相似文献   

15.
在室温下,测量了Er:Tm:NaY(WO4)2晶体的吸收光谱、激发光谱、发射光谱以及上转换发光,并运用J-O理论对测量的结果进行了计算,得出了Er:Tm:NaY(WO4)2晶体的强度参数.报道了Tm,Er离子间特殊的能量传递和相关上转换,解释了离子间的能级跃迁过程.同时,对于Er增强Tm离子近红外发光的特性也作了充分研究. 关键词: 4)2晶体')" href="#">Er:Tm:NaY(WO4)2晶体 吸收光谱 发射光谱 激发光谱 上转换  相似文献   

16.
孟庆裕  刘志鑫  孙文军* 《物理学报》2013,62(9):97801-097801
采用共沉淀法制备了不同Eu3+掺杂浓度的Gd2(WO4)3纳米发光材料. 测量了纳米材料样品的X射线衍射谱(XRD) 和场发射扫描电镜, 对样品的结构和形貌进行了表征. 测量了各样品的发射光谱和激发光谱(声子边带光谱), 绘制了浓度猝灭曲线, 确定了最佳的掺杂浓度为20 mol%. 通过声子边带光谱计算了不同掺杂浓度样品的黄昆因子. 测量了不同浓度样品的荧光寿命, 利用Auzel模型对Eu3+ 5D0能级荧光寿命数据进行了拟合, 确定了5D0能级的固有寿命和猝灭过程中生成的声子数. 本文还根据荧光寿命数据计算了Eu3+之间的能量传递速率, 确定了能量传递速率与浓度的关系. 关键词: 钨酸盐 3+')" href="#">Eu3+ 黄昆因子 能量传递速率  相似文献   

17.
Non-radiative energy transfers (ET) from Ce3+ to Pr3+ in Y3Al5O12:Ce3+, Pr3+ and from Sm3+ to Eu3+ in CaMoO4:Sm3+, Eu3+ are studied based on photoluminescence spectroscopy and fluorescence decay patterns. The result indicates an electric dipole-dipole interaction that governs ET in the LED phosphors. For Ce3+ concentration of 0.01 in YAG:Ce3+, Pr3+, the rate constant and critical distance are evaluated to be 4.5×10−36 cm6 s−1 and 0.81 nm, respectively. An increase in the red emission line of Pr3+ relative to the yellow emission band of Ce3+, on increasing Ce3+ concentration is observed. This behavior is attributed to the increase of spectral overlap integrals between Ce3+ emission and Pr3+ excitation due to the fact that the yellow band shifts to the red spectral side with increasing Ce3+ concentration. In CaMoO4:Sm3+, Eu3+, Sm3+-Eu3+ transfer occurs from 4G5/2 of Sm3+ to 5D0 of Eu3+. The rate constant of 8.5×10−40 cm6 s−1 and the critical transfer distance of 0.89 nm are evaluated.  相似文献   

18.
Shaped single crystals of (LuxGd1−x)3Ga5O12 (0.0x1.0) and (Yb0.05LuxGd0.95−x)3Ga5O12 (0.0x0.9) were grown by the modified micro-pulling-down method. Continuous solid solutions with garnet structure and a linear compositional dependency of crystal lattice parameter in the system Yb:(Gd,Lu)3Ga5O12 are formed. Measured optical absorption spectra of the samples show 4f–4f transitions related to Gd3+ ion at 275 and 310 nm, and also an onset of charge transfer transitions from oxygen ligands to Gd3+ or Yb3+ cations below 240 nm. A complete absence of Yb3+ charge transfer luminescence under X-ray excitation in any of the investigated samples was explained by the overlapping of charge transfer absorption of Yb3+ by that of Gd3+ ions. For specific composition of Lu1.5Gd1.5Ga5O12 an intense defect-host lattice-related emission, which achieve of about 40% integrated intensity compared with Bi4Ge3O12, was found.  相似文献   

19.
The emission properties of Eu2+ and Mn2+ in monoclinic SrAl2Si2O8 (M-SAS) and hexagonal BaAl2Si2O8 (H-BAS), both of which have only one alkaline-earth site, were studied. The emission peaks of both Eu2+ (405 nm) and Mn2+ (564 nm) in SrAl2Si2O8, are located at longer wavelengths, compared with those in H-BAS (373 nm for Eu2+ and 518 nm for Mn2+), because of the stronger crystal field strength at the Sr site. EPR spectra showed that the g values of Mn2+ are 4.5065 in M-SAS:Mn and 2.0247 in H-BAS:Mn. Magnetic measurements proved that Mn2+ was at high-spin state in both hosts. The large g value of Mn2+ in M-SAS was ascribed to the mixing of the first excitation state to the ground state, both of which have lower d orbital degeneracy due to the lower symmetry of Mn2+ site. The transfer efficiency from Eu2+ to Mn2+was about 10% in M-SAS, higher than that in H-BAS (5%). This was probably because Eu2+ emission overlaps the relatively low excitation level of Mn2+ in M-SAS. In order to obtain high transfer efficiency, it was necessary for the Eu2+ emission to overlap the lowest excitation level of Mn2+. The results obtained in this work may be helpful to design the new white or red phosphors for white-light emitting diode (w-LED) applications.  相似文献   

20.
Two potassium rare-earth polyphosphate single-crystals KLn(PO3)4 (Ln=Ce (1), Eu (2)) have been synthesized by the high-temperature solution reaction and characterized by single-crystal X-ray diffraction. The two isostructural compounds crystallize in the monoclinic system with space group P21, and all cell parameters shrink with the decrease of Ln3+ ion radius. The main structural feature is (PO3)44− wavy chains and infinite tunnels delimited by LnO8 and KO8 polyhedra. The energy band structures, density of states (DOS), and optical response functions for 1 have been calculated with the density functional theory (DFT) method, and the dielectric functions and refractive indices have been discussed. The measurements of the absorption and emission spectra show that 1 exhibits the ultraviolet emissions, and 2 displays the characteristic yellow-red emissions of Eu3+.  相似文献   

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