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1.
按摩尔百分比制备了组分为30SiO2-(20-x-y)Al2O3-40PbF2-10CdF2-xTm2O3-yYb2O3的两组Tm3+/Yb3+共掺杂氟氧硅铝酸盐上转换蓝色发光玻璃陶瓷材料,测量了其在980nm激 关键词: 玻璃陶瓷 上转换发光 3+/Yb3+掺杂')" href="#">Tm3+/Yb3+掺杂 掺杂浓度  相似文献   

2.
Energy transfer processes were studied in two sets of Yb3+ and Tm3+ co-doped sodium-metaphosphate glasses, prepared in air and nitrogen atmospheres. Using Förster, Dexter, and Miyakawa theoretical models, the energy transfer parameters were calculated. The main ion–ion energy transfer processes analyzed were energy migration among Yb3+ ions, cross-relaxations between Yb3+ and Tm3+ ions, and interactions with OH? radicals. The results indicated that Yb→Tm energy transfer favors 1.8 μm emissions, and there is no evidence of concentration quenching up to 2% Tm2O3 doping. As expected, samples prepared in nitrogen atmosphere present higher fluorescence quantum efficiency than those prepared in air, and this feature is specially noted in the near-infrared region, where the interaction with the OH? radicals is more pronounced.  相似文献   

3.
The Y2O3:R(R = Yb3+, Er3+, Tm3+) nanophosphors were synthesized by a solvothermal method and the temperature dependence of the white upconversion emission was studied using a 975 nm LD. The upconversion emission spectra in 1 mol% Er3+/5 mol% Yb3+/xTm3+ tri-doped Y2O3 nanophosphors were sintered at 1000 °C with x from 0 to 0.5 mol%. The blue emission intensity increases increasing Tm3+ concentration from 0 to 0.5 mol%, because the Tm3+ state can be easily reached due to the 2F7/2 → 2F5/2 transition of Yb3+ near 10,000 cm−1. The Y2O3: Er3+/Yb3+/Tm3+ nanophosphors exhibit upconversion emission from white to green with increasing sintering temperature. The calculated CIE coordinates are located in the white region at a pump power of 700 mW at 1000 °C, and the color coordinates were very similar to the standard white light emission. Their upconversion process was described through energy level diagrams and results of upconversion emission spectra and pump power dependence.  相似文献   

4.
郭琳娜  王育华 《物理学报》2011,60(2):27803-027803
采用化学共沉淀法制备了系列Y1.98-2xYb2x Er0.02SiO5(0.00≤x≤0.15)以及Y1.736Yb0.24Er0.02Tm0.004SiO5上转换发光材料,比较了室温下Y1.98-2xYb2x Er0.02 SiO5 (x=0.00,0.08)样品在400—1600 nm范围内的吸收光谱,测量了所有样品在976 nm OPO激光器激发下的上转换发射光谱,以及Er3+离子4S3/2(4F9/2)→4I15/2,Tm3+离子1G43H6荧光衰减曲线和不同激发功率下的上转换蓝光发射强度,从而分析讨论了Er3+,Tm3+在Y2SiO5中的上转换发光机理.研究结果表明:在1250 ℃相对较低的温度下合成了X2型单斜晶系Y2SiO5 ∶Ln3+(Ln3+=Er3+,Yb3+,Tm3+),Yb3+的敏化显著增强了样品在976 nm附近的吸收能力,并大幅度加宽了该处的吸收带.分析上转换发射光谱发现:上转换绿光和红光强度都随着Yb3+浓度的增加先增强后减弱,但红光的猝灭浓度较高,归因于Er3+→Yb3+反向能量传递ETU4和Yb3+→Er3+正向能量传递ETU3过程的发生;上转换蓝光发射是三光子吸收过程,是通过Yb3+,Tm3+之间三次声子辅助的能量转移方式实现的. 关键词: 上转换 共沉淀 2SiO5∶Er3+')" href="#">Y2SiO5∶Er3+ 3+')" href="#">Yb3+ 3+')" href="#">Tm3+  相似文献   

5.
Strontium aluminate (SrAl4O7) nanophosphor codoped with Tm3+–Yb3+ has been synthesized through the combustion route using urea as the reducing agent. Structural, thermal and optical characterizations have been carried out. Heat treatment of the samples shows a change in the crystallite phases and the relative luminescence intensities for the different bands. The nanocrystalline particles in the as-synthesized sample seem to arrange in rod like shapes of submicrometer length on annealing. A broad (350–550 nm) emission in the UV–green region is observed when 266 nm radiation is used for excitation. Intense upconversion (UC) emissions in blue, red and infrared are seen with excitation by 976 nm radiation. An emission at 364 nm not observed earlier and attributed to 1D23H6 transition in Tm3+ is also seen. The blue emission from SrAl4O7:Tm3+/Yb3+ codoped nanophosphor (annealed at 1200°C) exhibits high color purity (89%) and is comparable to phosphors used commercially. The energy transfer mechanisms, responsible for these UC emissions, are proposed and discussed.  相似文献   

6.
Near-infrared excited up-conversion phosphors of RE3+/Yb3+(RE = Ho, Tm) co-doped SrIn2O4 were synthesized by a solid-state reaction method. X-ray diffraction analysis revealed the phase composition of those samples, and the up-conversion spectroscopic properties were studied in terms of up-conversion emission spectra. Under 980 nm near-infrared laser excitation, strong green emission with the peak at 546 nm was observed in SrIn2O4: Ho3+/Yb3+, which can be assigned to the characteristic 5S2(5F4)  5I8 transition of Ho3+. Furthermore, SrIn2O4: Tm3+/Yb3+ showed bright blue emission with the peak at 486 nm, which is associated with the 1G4  3H6 transition of Tm3+. The UC power studies indicated that the luminescence of SrIn2O4: Ho3+/Yb3+ and SrIn2O4: Tm3+/Yb3+ are attributed to two-photon and three-photon process, respectively. The possible UC luminescence mechanism and energy transfer in SrIn2O4: RE3+/Yb3+ were discussed.  相似文献   

7.
Tm3+/Yb3+共掺氧卤碲酸盐玻璃上转换发光研究   总被引:1,自引:0,他引:1       下载免费PDF全文
研究了Tm3+/Yb3+共掺氧卤碲酸盐玻璃的上转换发光光谱,分析了Tm2O3含量对Tm3+/Yb3+共掺氧卤碲酸盐玻璃上转换发光的影响机理.结果表明:在Tm3+/Yb3+共掺氧卤碲酸盐玻璃的上转换发光中,Tm3+存在较强的浓度猝灭效应.随Tm2O3含量增加,Tm3+的上转换蓝光和红光强度先增加,后降低,在0.1mol% Tm2O3达到最大.该结果有助于进一步提高Tm3+的上转换发光效率.  相似文献   

8.
This work reports the upconversion luminescence properties of Tm3+/Yb3+ ions in lead tungstate tellurite (LTT) glasses. Judd–Oflet intensity parameters have been obtained from the absorption band intensities of Tm3+ singly-doped and Tm3+/Yb3+ co-doped LTT glasses. The spontaneous emission probabilities, radiative lifetimes and branching ratios for 1G4 and 3H4 emission levels of Tm3+ have been determined. Upconversion luminescence has been observed by exciting the samples at 980 nm (Yb3+:2F7/22F5/2) at room temperature. Four upconversion emission bands corresponding to the 1G43H6 (477 nm), 1G43F4 (651 nm), 1G43H5 (702 nm) and 3H43H6 (810 nm) transitions have been identified. The relative variation in the intensities of upconversion bands, the different channels responsible for upconversion spectra and the effect of Yb3+ ions concentration on the upconversion luminescence of Tm3+ ions have also been discussed.  相似文献   

9.
The excitation and emission properties of the lanthanides Ce3+, Pr3+, Nd3+, Sm3+, Eu3+, Tb3+, Er3+, Tm3+, and Yb3+ in LiYP4O12 were studied by vacuum ultra-violet spectroscopy at 10 K. It provides information on the energies of 4f-5d excitation and emission bands. In the case of Er3+ spin forbidden emission was observed. Charge transfer excitation bands were identified for Eu3+, Sm3+, Tm3+, and Yb3+, and in the case of Yb3+ charge transfer luminescence is observed. All data appear to be consistent with each other and have been used to construct a level scheme showing the location of the energy levels of all trivalent and divalent lanthanides in LiYP4O12.  相似文献   

10.
The spectroscopic investigation of Tm3+ or (Nd, Yb, Tm)-doped Sc2O3 transparent ceramics, as laser-active media for visible and IR emission, was performed. The spectra are dominated by Tm3+ ions in sites of C2 symmetry and an energy level scheme and other spectral parameters were determined. The strong concentration quenching of 3H4 level emission in Tm:Sc2O3 at 300 K is discussed by considering the resonant cross-relaxation (3H43F4)?(3H63F4) process and multipolar interactions of various orders. The main energy-transfer processes leading to the blue upconversion emission from the 1G4 Tm3+ level in (Tm, Nd, Yb):Sc2O3 ceramic, under pulsed pumping at 808.3 nm were evidenced.  相似文献   

11.
Tm3+/Yb3+ codoped tellurite glass has been prepared. Density, refractive index, optical absorption, Judd-Ofelt parameters and spontaneous transition probabilities of Tm3+ have been measured and calculated, respectively. Intense blue three-photon upconversion fluorescence and S-band (1470 nm) fluorescence were investigated under the excitation of a 980 nm diode laser at room temperature. Judd-Ofelt parameters, strong blue three-photon upcoversion emission of Tm3+ in glass indicate that Tm3+/Yb3+ codoped tellurite glass is a promising blue color upconversion optical and laser material. In addition, experiment results showed the 980 nm laser was more efficient than 808 nm laser when pumping Tm3+/Yb3+ codoped tellurite glass, Tm3+/Yb3+ codoped tellurite glass also could be a promising material for S-band amplification.  相似文献   

12.
Desvitrification in a Tm3+ and Yb3+ codoped oxyfluoride glass has been obtained by exciting with a continuous Argon laser radiation increasing the average laser power from 144 to 2900 mW. Excitation spectra inside a locally damaged zone in a 1 mol% Tm3+ and 2.5 mol% Yb3+ codoped glass have been measured under excitation in the wavelength range 750–830 nm detecting the 2F5/2 (Yb3+) level. This curve is the result of the contribution of two different kinds of centers, the fluoride nanocrystals and the glassy phase of the glass ceramic sample created due to the irradiation. The weight of the contributions of each of the centers depends on the excitation wavelength, and from the analysis of the decay of the luminescence it can be concluded that approximately 80% of the Tm3+ ions are located in the nanocrystals and therefore less than 20% in the glassy phase.  相似文献   

13.
The YAG nanopowders were prepared by a co-precipitation method using nitrate and ammonium hydrogen carbonate as raw materials. To obtain homogenous precipitate, reverse-strike (adding salt solutions to the precipitant solution) technique was adopted. Therefore, single (Tm3+) and codoped (Tm3+–Yb3+) YAG nanopowders with a size between 40–90 nm have been obtained.Blue upconversion emission at around 480 nm has been found in YAG: Tm3+ nanopowders under excitation to the 3H4 level of Tm3+ at around 800 nm. However, this upconversion emission in nanopowders codoped with Tm3+–Yb3+ ions is increased by a factor of about 10. The analysis of the temporal evolution of the involved levels and the dependence of the upconversion intensity on the pump power at 800 nm allowed to distinguish the upconversion mechanism. In YAG: Tm3+ nanopowders the upconversion mechanism is due to excited state absorption processes. However, in the codoped samples, Yb3+ ions acts as the sensitizers; in consequence, the blue upconversion is strongly increased.  相似文献   

14.
Tm3+/Yb3+ co-doped Y2O3 nanophosphor has been synthesized by the solution combustion technique. Heat treatment of the phosphor materials at higher temperatures modifies the structural and optical properties. At low concentration of Yb3+, an intense upconversion emission is observed in blue region (478?nm) on excitation with 976?nm radiations. Emission has also been observed in the ultraviolet (UV) region viz. at 300?nm. The intensity of blue emission initially increases with dopant concentration as well as with the annealing temperature. However, for higher concentrations of Yb3+ (10?mol%), emission in the blue region is greatly suppressed and NIR emission at 813?nm appears with a large intensity. Intensity ratio of NIR and blue emission (I NIR/I B) reaches 74, resulting in almost monochromatic light at 813?nm. To check the suitability of blue emission for display devices, CIE color coordinates (x,y), color purity and the dominant wavelength (?? d) for the blue emission have been calculated and the resulting value is found to be close to the coordinates of available standard blue phosphors.  相似文献   

15.
用高温熔融法制备了Tm3+/Ho3+/Yb3+共掺碲酸盐玻璃(TeO2-ZnO-La2O3)样品,测试了玻璃样品的吸收光谱和上转换发光光谱,分析了上转换发光机理.结果发现:在975 nm波长激光二极管(LD)激励下,制备的碲酸盐玻璃样品可以观察到强烈的红光(662 nm)、绿光(546 nm)和蓝光(480 nm)三基色上转换发光,红光对应于Tm3+离子 关键词: 碲酸盐玻璃 上转换发光 白光 3+/Ho3+/Yb3+共掺')" href="#">Tm3+/Ho3+/Yb3+共掺  相似文献   

16.
共沉淀法制备NaYF4 : Tm3+,Yb3+的上转换发光   总被引:4,自引:3,他引:1       下载免费PDF全文
通过共沉淀法制备Tm3+和Yb3+掺杂的NaYF4上转换发光材料。其中Tm3+和Yb3+的摩尔分数分别为0.01%,0.1%。在室温下测试了NaYF4 : Tm3+,Yb3+材料在300~1 100 nm的吸收光谱。利用X射线衍射(XRD),扫描电镜(SEM)测试了合成材料的物相结构和微观形貌。结果表明:NaYF4 : Tm3+,Yb3+材料为六方相晶体,其颗粒大小约为50~60 nm,产物结晶良好,含有少量杂相。在798 nm近红外光激发下,测试了样品的上转换发光光谱。观察到了蓝、绿色上转换发光。讨论了上转换发光的可能机理,蓝光主要来源于Tm3+的激发态1G4到基态3H6的跃迁,绿光来源于Tm3+1D23H5跃迁。  相似文献   

17.
Abstract

We present the Raman spectrum of Tm3Al5O12 single crystal and its pressure dependence for hydrostatic pressure up to 11GPa and room temperature. Tm3Al5O12 belongs to the crystal family of rare earth garnets (Re3A12(AlO4)3, Re: Gd, Tb, Dy, Er,…), which crystallize in the body-centered cubic lattice and contains eight molecular units in the conventional unit cell, Group theory predicts 25 Raman active modes for these compounds, while experimentally are observed 15 modes. As crystal volume decreases all Raman peaks exhibit pressure coefficients varying from 0.7 to 5.6cm?1/ GPa. A large part of the vibrational spectra of these compounds could be explained taking into account the vibrational properties of molecular subunits, namely AlO4.  相似文献   

18.
Tm3+-Eu3+ energy transfer processes and relaxation dynamics of the 3 H 4 and 3 F 4 excited states of Tm3+ ions in 1 at. % Tm3+, 5 at. % Eu3+:YVO4 single crystal were studied. Contribution of Tm3+-Eu3+ energy transfer reduces effectively the lifetime of terminal level in a potential 3 H 43 F 4 laser transition at around 1.48 μm. Adverse quenching of the 3 H 4 emission by Eu3+ ions is found to be less efficient than that reported for Tm3+ + Tb3+ system in YVO4. The classical Inokuti–Hirayama model accounts well for an experimental decay curve of the 3 H 4 emission recorded for co-doped crystal. Stimulated emission cross section for 3 H 43 F 4 transition of Tm3+ at around 1.48 μm was analyzed taking into account the anisotropy of YVO4 crystal. PACS 42.55.Xi; 42.62.Fi  相似文献   

19.
The Ho3+/Yb3+ and Tm3+/Yb3+ doped P2O5-MgO2-Sb2O3-MnO2-AgO glasses were prepared by high temperature melting method. Under a 975 nm laser diode (LD) excitation, the single red and single blue upconversion (UC) emissions were observed in Ho3+/Yb3+ and Tm3+/Yb3+ doped samples, respectively. By studying the spontaneous radiative and multiphonon relaxation probabilities, we find that the multiphonon relaxation probability of 5I6 (Ho3+) state is very large (1.39 × 106 s− 1), which is helpful to the population of 5I7 state. The multiphonon relaxation probability of 3H5 and 3F2,3 (Tm3+) is also very large, which results in lots of population in 3F4 and 3H4 states. The results are that the red UC emission of Ho3+ and the blue UC emission of Tm3+ are stronger.  相似文献   

20.
Q Fu  S Y Wu  J Z Lin  J S Yao 《Pramana》2007,68(3):499-506
The impurity displacements for Fe3+ and Ru3+ in corundum (Al2O3) are theoretically studied using the perturbation formulas of the spin Hamiltonian parameters (zero-field splitting and anisotropic g factors) for a 3d5 (with high spin S = 5/2) and a 4d5 (with low spin S = 1/2) ion in trigonal symmetry, respectively. According to the investigations, the nd5 (n = 3 and 4) impurity ions may not locate at the ideal Al3+ site but undergo axial displacements by about 0.132 Å and 0.170 Å for Fe3+ and Ru3+, respectively, away from the center of the ligand octahedron along the C3 axis. The calculated spin Hamiltonian parameters based on the above axial displacements show good agreement with the observed values. The validity of the results is discussed.  相似文献   

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