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1.
To obtain efficient upconversion laser glass, the optical properties of Tm3+ and Ho3+ were investigated in various glasses. Fluoride glass was selected as base glass for upconversion. The efficient upconversion fluorescences corresponding to the 1G43H6 and 3H43H6 transitions of Tm3+ and the 5S25I8 transition of Ho3+ were observed in Yb3+-Tm3+ and Yb3+-Ho3+ doped aluminozircofluoride glasses excited at 980 nm. The very stronge blue and green emission light can be observed visually. The upconversion processes observed were two-photon processes for 3F43H6, 5S25I8 transitions and three-photon processes for the 1G43H6 transition and can be described by a rate equation model. The energy transfer and energy back-transfer were analyzed in Yb3+-Tm3+ and Yb3+-Ho3+ systems. The relationship between emission intensity, pumping intensity and dopant concentrations is described using a rate equation model and shows good agreement with experiments. The dynamics of excited state ( ) is also analyzed with the diffusion-limited model based on Yokota-Tanimoto theory.  相似文献   

2.
The optical properties of the rare elements Tm3+, Ho3+ and Yb3+ were systematically investigated in various glasses. The Tm3+ doped aluminozircofluoride glass shows higher quantum efficiency, longer lifetime and stronger fluorescence intensity than Tm3+ doped YSGG crystal and other Tm3+ doped glasses for the 3H43H6 transition. Similar quantum efficiency, longer lifetime and stronger fluorescence intensity were also found in Ho3+ doped aluminozircofluoride glass for the 5I75I8 transition. The higher quantum efficiencies of Tm3+ and Ho3+ in aluminozircofluoride glass are due to the longer lifetime and the lower phonon energy. The fluorescence mechanisms and energy transfer in the Yb3+ -Tm3+ system, Yb3+ -Ho3+ system and Yb3+ - Tm3+ -Ho3+ system were studied. The very strong fluorescence intensities in the Yb3+ -Tm3+ system for Tm3+ and the Yb3+ -Tm3+ -Ho3+ system for Ho3+ which are 1.68 times that of Tm3+ doped YSGG crystal and 2.25 times that of Tm3+---Ho3+ codoped YSGG crystal are attributed to the efficient Yb3+ → Tm3+, Yb3+ → Ho3+ and Tm3+ → Ho3+ energy transfer processes. The fluorescence processes are described by cross relaxations of 2F5/23H53H43H62F7/2 and2F5/23H5 (or 2F5/25I63H5) → 3H45I75I83H62F7/2.  相似文献   

3.
Rare earth ion (Nd3+, Er3+ and Tb3+)-doped alumina films were prepared by the sol–gel method using aqueous alumina sol. The effects of dopant concentration and treatment temperature on the optical properties, absorption and emission were examined for the doped films. Alumina films prepared by this method gave a high dopant concentration (0–15 mol% per alumina). Significant concentration quenching did not occur in this concentration range. The emissions from 5D3 and 5D4 of Tb3+-doped film reflected sensitively a matrix environment around Tb3+ ions. Er3+- and Nd3+-doped alumina films resonantly excited by cw Ti–sapphire laser (800 nm) showed upconversion emission at room temperature. The former gave 548 nm (4S3/24I15/2) and 640 nm (4F9/24I11/2) signals, and the latter 640 nm (4G7/24I11/2), which were dependent on alumina.  相似文献   

4.
用高温熔融法制备了Bi、Tm、Bi/Tm掺杂TiO2-BaO-SiO2-Ga2O3玻璃系统。在808 nm激光激发下, 与Tm单掺杂玻璃相比, Bi/Tm共掺玻璃中Tm3+3H43F4跃迁荧光(~1485 nm)得到了显著的增强, 而Tm3+3F43H6跃迁荧光(~1810 nm)减弱。在980 nm激光激发下, Tm单掺玻璃中没有观察到Tm离子的特征发光, 而在Bi/Tm共掺玻璃中观察到Tm3+3F43H6跃迁荧光(~1810 nm)。这是由于在808和980 nm激光二极管(LD)各自激发下, Bi/Tm共掺玻璃中活性Bi离子的近红外发光能量传递给Tm3+, 分别产生3F43H43H63H5跃迁所致。采用Inokuti-Hirayama模型, 分析了该玻璃体系中Bi→Tm的能量传递机理。结果表明, Bi→Tm的能量传递属于电偶极–偶极相互作用。  相似文献   

5.
The temperature dependencies of the nanosecond multiphonon relaxation (MR) rates of the 3F3 state of Tm3+ in the YLF crystal and of the 5F5 state of Ho3+ ion in the YAG and LuAG crystals and of the microsecond MR rates of the 4F9/2 (2H9/2) state of Er3+ ions in YLF were measured in the wide temperature range using direct laser excitation and selective fluorescence kinetics decay registration. For YLF the observed relations are explained by 4-phonon process in the frame of a single-frequency model with hωeff=450±30 cm−1 for the 3F3 state of Tm3+ and by 5-phonon process with hωeff=445 cm−1 for the 4F9/2 (2H9/2) state of Er3+. For YAG and LuAG crystals these dependencies are explained by the 3-phonon process with hωeff=630 cm−1. The decrease of the relaxation rate with the temperature in the range from 13 to 80 K was observed for the 4F9/2 (2H9/2) state of Er3+ in the YLF crystal. It is explained by the redistribution of excited electronic states population of erbium ions over the higher lying Stark levels with different MR probabilities. A good fit of experimental temperature dependence (including the dropping part of the experimental curve) was obtained for single-frequency model (hωeff=450 cm−1) with W01=8.0×104 s−1 and W02=4.7×104 s−1 accounting Boltzmann distribution of population over two excited Stark levels of the excited state of erbium ions. Employment of this model improves the fit between the experiment and the theory for the 5F5 state of Ho3+ ion in YAG as well. Strong influence of the parameters of the non-linear theory of MR, i.e. the reduced matrix elements U(k) of electronic transitions and the phonon factor of crystal matrix η on the spontaneous MR rates was observed experimentally. The smaller these parameters the slower the spontaneous MR W0. This fact can be used for searching new active crystal laser media for the mid-IR generation.  相似文献   

6.
Hai Guo   《Optical Materials》2007,29(12):1840-1843
In this work, the LaOBr:Er3+ (0.1%) powders were prepared by solid state reaction. The structural properties of LaOBr:Er3+ were characterized by X-ray diffraction (XRD), Fourier transform infrared spectroscopy (FT-IR) and Raman spectroscopy. The results show that LaOBr:Er3+ has low phonon energy, which indicate that LaOBr:Er3+ may have high luminescent efficiency. Under excitation into 4I11/2 level of Er3+ ions by 980 nm laser, the two- and three-photon upconverted luminescence of LaOBr:Er3+ were recorded. The most intense emissions were come from the 2H11/2, 4S3/2 → 4I15/2 transitions. The upconversion mechanisms were studied in detail through laser power dependence, and results show that excited state absorption is responsible for the upconversion. The upconversion properties indicate that LaOBr:Er3+ may be used in upconversion phosphors.  相似文献   

7.
采用水热法合成了Yb3+-Tm3+共掺BiOBr纳米晶, 研究了其上转换发光性能。在980 nm光激发下, 样品中Tm3+离子实现了3H43H61G43F41G43H6跃迁, 进而发出强烈的近红外光(801 nm)和较弱的红光(655 nm)与蓝光(485 nm)。探讨了样品的上转换发光机理, 上转换发光强度与激发功率的关系表明在980 nm激发下Tm3+的蓝光和红光发射为三光子过程, 而近红外发光为双光子过程。随着Yb3+浓度增加, 近红外发光显著增强, 近红外光与蓝光(I801 nm/I485 nm)的发光强度比高达71.4。研究结果表明, Yb3+-Tm3+共掺BiOBr纳米晶在生物荧光标记领域具有潜在的应用前景。  相似文献   

8.
先用液相沉淀技术合成Lu/In/Tm/Yb四元体系水合碱式碳酸盐类沉淀前驱体,然后将其在1100℃煅烧制备出一系列类球状平均粒度约为110 nm的[(Lu0.5In0.5)0.999-xTm0.001Ybx]2O3 (x=0~0.05)氧化物固溶体。在980 nm泵浦激光激励下这种氧化物粉体在可见光区发射出强烈的蓝青光(450~510 nm,源于Tm3+离子4f12电子组态内1D23H6,3F4电子跃迁)和较弱的红光(650~670 nm,源于Tm3+离子的1G43F4电子跃迁),二者的上转换过程均为双光子吸收。随着Yb3+离子浓度的提高1931CIE色坐标上的发射光颜色逐渐由绿光(0.31, 0.54)移向蓝光(0.01, 0.19)。Yb3+离子共掺提高了Tm3+离子的上转换发光强度,其最佳含量为2.5%。发射474 nm蓝光和654 nm红光的粉体,其荧光寿命分别约为0.84和0.97 ms。  相似文献   

9.
戴智刚  李友芬  李刚  杨儒 《无机材料学报》2016,31(10):1081-1086
采用高温固相法合成了Tb3+, Yb3+共掺杂的Sr2B2O5荧光粉。通过X射线衍射(XRD)和荧光光谱(PL)对样品的物相结构和发光性质进行了表征。XRD结果表明, 合成样品为单斜结构的Sr2B2O5相。分别使用543 nm和980 nm的监测波长, 得到的激发光谱均在354 nm、374 nm处有较强的激发峰, 其中374 nm处最强, 说明Sr2B2O5荧光材料在近紫外光区对太阳光有很强的吸收; 在374 nm( Tb3+:7F65D3) 紫外光激发下, 观察到Tb3+: 5D47FJ ( J = 6, 5, 4, 3) 可见光区发射光, 并检测到Yb3+: 2F5/22F7/2的近红外发射光。通过研究激发光谱和发射光谱与Yb3+掺杂浓度的关系, 发现在单斜晶体Sr2B2O5中, Yb3+具有很高的猝灭浓度。  相似文献   

10.
Water soluble upconversion (UC) luminescence hexagonal-phase NaGdF4: Yb3+/Tm3+ nanoparticles have been successfully synthesized by the hydrothermal method. XRD, SEM, UC photoluminescence spectra and electron paramagnetic resonance (EPR) spectrum were used to characterize the nanoparticles. The intensity of UC emission region could be controlled through different sodium source and the fluorine source, 6PJ8S7/2 emission of Gd3+ is also observed at 310 nm. A broad spectrum with a dominant resonance at g of about 2 was observed by the EPR spectrum of the NaGdF4:Yb3+/Tm3+ nanoparticles. The transparent NaGdF4:Yb3+/Tm3+ solution presented naked eye-visible violet-blue light under the 980 nm LD excitation. The current work paves the way for their potential application in infrared tomography and magnetic resonance imaging (MRI).  相似文献   

11.
上转换纳米颗粒因具有良好的穿透深度和发光强度被广泛地应用在生物标记或生物成像中。实验制备了核壳结构的NaYF4:Yb@NaYF4:Ho纳米颗粒, 分散均匀, 粒径在50 nm左右。通过光谱分析可知, 该纳米颗粒可在980 nm激光激发下发射波长为650 nm为主的发射光。进一步对该核壳结构的NaYF4:Yb@NaYF4:Ho纳米颗粒进行Nd3+掺杂, 制备了可被800 nm激光激发且发射强红光的纳米颗粒。通过比较多种不同结构的Nd3+掺杂NaYF4:Yb@NaYF4:Ho纳米颗粒的荧光光谱发现, NaYF4:Yb@NaYF4:Ho,Nd纳米颗粒发射光最强, 表明Nd3+掺杂在NaYF4:Yb@NaYF4:Ho纳米颗粒的壳层中最佳。最后对NaYF4:Yb3+50%@NaYF4:Ho3+1%,Nd3+x%纳米颗粒Nd3+离子的掺杂浓度进行优化, 实验结果表明: Nd3+掺杂浓度为30%时,该纳米颗粒在800 nm激光激发下发光强度最强。  相似文献   

12.
曲姣  朱琦  李继光  孙旭东 《无机材料学报》2016,31(10):1087-1093
结合籽晶法和添加矿化剂硝酸铵, 通过均相沉淀合成和后续煅烧实现了(Y, Eu)2O3单分散球形颗粒(直径范围110~550 nm)的可控合成。通过XRD、FE-SEM、TEM和PLE/PL分析等手段对产物进行了系统表征。发现采用籽晶法和添加矿化剂硝酸铵可以促进球形颗粒长大。碱式碳酸盐前驱体经600℃煅烧分解为立方晶(Y, Eu)2O3, 且经1000℃煅烧后(Y, Eu)2O3依然继承球形形貌特征。所得多晶(Y, Eu)2O3球形荧光颗粒在242 nm激发下于615 nm处呈现最强红色荧光发射(Eu3+5D07F2跃迁)。荧光粉的荧光性能呈现明显的尺寸依存性。增大球形颗粒尺寸减小了荧光寿命(1.15~1.57 ms)和荧光不对称因子[I(5D07F2)/I(5D07F1)], 但增强了荧光发射强度。  相似文献   

13.
The synthesis and photoluminescent (PL) properties of calcium stannate crystals doped with europium grown by mechanically activated in a high energy vibro-mill have been investigated. The characteristics of Ca2SnO4:Eu3+ phosphors were found to depend on the amounts of europium ions. The XRD profiles revealed that the system, (Ca1−xEux)2SnO4, could form stable solid solutions in the composition range of x = 0–7% after being calcined at 1200 °C. The calcined powders emit bright red luminescence centered at 618 nm due to 5D0 → 7F2 electric dipole transition. Both XRD data and the emission ratio of (5D0 → 7F2)/(5D0 → 7F1) reveal that the site symmetry of Eu3+ ions decreases with increasing doping concentration. The maximum PL intensity has been obtained for 7 mol% concentration of Eu3+ in Ca2SnO4.  相似文献   

14.
Spectroscopic and EPR investigations of Nd3+-doped CaZn2Y2Ge3O12 (CAZGAR) have been performed. The absorption, fluorescence, excitation spectra and fluorescence lifetime have been measured at room temperature. The Judd-Ofelt theory has been applied to the measured optical absorption intensities to predict the radiative decay rates, branching ratios, and peak stimulated emission cross section from the metastable 4F3/2 state to the 4I9/2 manifold. The fluorescence lifetime of the 4F3/2 level of Nd3+ at low concentration in this host was measured to be 285 ± 10 μs, which is longer than that for Nd3+: YAG. Color centers located at zinc octahedral sites have been produced in these crystals by ultraviolet irradiation and have been detected by EPR techniques. The effects of the color centers on the potential laser characteristics of this materials are discussed.  相似文献   

15.
采用溶胶-凝胶法结合静电纺丝技术制备了柔性Eu3+掺杂SiO2纤维薄膜, 采用SEM、XRD、FT-IR、TG和PL等测试方法对材料进行表征。Eu3+掺杂SiO2纤维薄膜在热处理后纤维直径变小, 纤维表面平滑无粘连。通过控制升温速度, 纤维薄膜经热处理后仍具有较高的力学强度, 750℃热处理后其拉伸强度可达4.31 MPa, 经过多次弯曲仍能保持原样。在392.6 nm光源激发下, Eu3+掺杂SiO2纤维薄膜在570~670 nm附近呈现出来自于5D07FJ的发射峰。当Eu3+掺杂浓度为8mol%时, 经过750℃热处理后Eu3+掺杂SiO2纤维薄膜的发光强度达到最大值。  相似文献   

16.
Here, we bring out an infrared transmitting new optical glass based on TeO2 added with AlF3 and LiF, containing dual rare earth ions (Eu3+,Nd3+) as the dopants with a purpose to examine their luminescence and also the decay times pertaining to a prominent transition of Eu3+ (5D0 → 7F2 at 615 nm) as a function of temperature both in the presence and absence of Nd3+ ions. The energy transfer rates (Wtr), critical distances (R0) and transfer efficiencies (ηtr) have been evaluated based on the measured lifetime data of this glass.  相似文献   

17.
Lu2O3是具有高热导率而成为极具潜力的高功率激光介质材料。实验以商用氧化物粉体为原料, LiF为烧结助剂, 采用放电等离子烧结法制备了不同Nd3+掺杂浓度(CNd=0, 1at%, 3at%和5at%) Lu2O3透明陶瓷, 并研究了Nd3+掺杂浓度对Lu2O3陶瓷的物相、烧结性能、微观结构及光学性能的影响。结果表明:在高Nd3+浓度(5at%)掺杂后烧结样品仍为纯Lu2O3相;Nd3+掺杂对Lu2O3陶瓷烧结性能及微观形貌的影响有限;所有样品最终均表现出高致密性(99.5%以上)和优异的透光性能, 其中3at% Nd3+:Lu2O3的透过率最高, 在1064和2000 nm处的透过率分别为82.7和83.2%。Nd3+:Lu2O3透明陶瓷的最强发射峰位于1076和1080 nm;且随着Nd3+掺杂浓度的增加, 荧光强度降低, 寿命变短, 发生浓度淬灭。  相似文献   

18.
In this paper, YLiF4 codoped with Tm3+ and Yb3+ ions was synthesized by hydrothermal method. Yb3+ concentration is fixed at 1.5%, and Tm3+ concentration is changed from 0.1 to 0.4%. Intense upconversion luminescence is observed when the samples are excited by 980 nm. The dependence of upconversion luminescence on Tm3+ concentrations is presented. The results show that upconversion luminescence increases with the Tm+ concentration and gets its peak at 0.3 mol%. Under the excitation of 980 nm, the blue emission of 479 nm and the red emission of 647 nm are both duo to two photons process, and the UV emission of 361 nm is attributed to the three photons process. We also analyse the upconversion mechanism and process.  相似文献   

19.
以Y2O3、Eu2O3、Bi(NO3)3·H2O、浓HNO3、偏钒酸铵、氨水、无水乙醇和一缩二乙二醇为原料,采用聚乙烯吡咯烷酮(PVP)辅助水热法合成YVO4: Eu3+, Bi3+纳米颗粒。使用X射线衍射(XRD)、扫描电镜(SEM)、红外光谱(IR)和荧光光谱(FL)等手段对产品进行了表征和分析。结果表明:合成的样品为YVO4: Eu3+, Bi3+纳米颗粒,均具有四方晶相结构,其微结构随反应溶液的的pH值变化。YVO4: Eu3+, Bi3+纳米颗粒在619 nm处有较强的红光发射(电偶极跃迁5D07F2),在594 nm有较弱的橙光发射(磁偶极跃迁5D07F1)。随着Eu/Bi比值的增大材料的荧光先增强后减弱,在Eu/Bi比值为5时样品的红光发射最强。溶液的pH值影响YVO4: Eu3+, Bi3+纳米晶的发光强度,其中pH值为10时的样品其红光发射最强。并探讨了YVO4: Eu3+, Bi3+纳米晶的发光机理。  相似文献   

20.
The blue phosphor of BaMgAl10O17:Eu2+ (BAM) powders were prepared by solid-state reaction. The thermal degradation of BAM phosphor significantly reduces the intensity of the blue emission. BAM is reduced by an amount of 50% after heating at around 800 °C for 1 h. Photoluminescence (PL) excitation and emission spectra showed that the blue emission of 450 nm peak decreased with increasing annealing temperature. The 5D07F1 and 5D07F2 transition of Eu3+ were observed at 590 and 615 nm emission lines over 1100 °C. Electron paramagnetic resonance (EPR) spectrum also detected two signals of Eu2+, corresponding to g=3.7156(9) for 88 mT, and g=2.9507(9) for 133 mT. X-ray absorption near edge structure (XANES) spectrum decreased the intensity of Eu2+ for 6977 eV with increasing annealing temperature, while high-energy peak of Eu3+ for 6984 eV was increased. The combined use of X-ray and neutron data by the Rietveld refinement appears to support that the secondary phase of EuMgAl11O19 magnetoplumbite structure in BAM may be formed by heat treatment.  相似文献   

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