944 resultados para Rare earth ions


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An interesting fluorescence intensity reverse photonic phenomenon between red and green fluorescence is investigated. The dynamic range. of intensity reverse between red and green fluorescence of Er( 0.5) Yb( 3): FOV oxyfluoride nanophase vitroceramics, when excited by 378.5nm and 522.5nm light respectively, is about 4.32 x 10(2). It is calculated that the phonon- assistant energy transfer rate of the electric multi- dipole interaction of {(4)G(11/2)( Er3+) -> F-4(9/2)( Er3+), F-2(7/2)( Yb3+). F-2(5/2)( Yb3+)} energy transfer of Er( 0.5) Yb( 3): FOV is around 1.380 x 10(8) s(-1), which is much larger than the relative multiphonon nonradiative relaxation rates 3.20 x 10(5) s(-1). That energy transfer rate for general material with same rare earth ion's concentration is about 1.194 x 10(5) s(-1). These are the reason to emerge the unusual intensity reverse phenomenon in Er( 0.5) Yb( 3): FOV. (C) 2007 Optical Society of America.

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Er3+, Yb3+ and Tm3+ codoped fluorophosphate glasses emitting blue, green and red upconversion luminescence at 970 nm laser diode excitation were studied. It was shown that Tm3+ behaves as the sensitizer to Er3+ for the green upconversion luminescence through the energy transfer process: Tm 3+:H-3(4) + Er3+:I-4(15/2) -> Er3+:I-4(9/2) + Tm3+:H-3(6), and for the red upconversion luminescence through the energy transfer process: Tm3+:F-3(4) + Er3+:I-4(11/2) -> TM3+:H-3(6) + Er3+:4 F-9/2. Moreover, Er3+ acts as quenching center for the blue upconversion luminescence of TM3+. The sensitization of Tm3+ to Er3+ depends on the concentration of Yb3+. The intensity of blue, green and red emissions can be changed by adjusting the concentrations of the three kinds of rare earth ions. This research may provide useful information for the development of high color and spatial resolution devices and white light simulation. (C) 2006 Elsevier B.V. All rights reserved.

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abstract {Rare earth ions doped multi-component glass fibers have important application in broad band fiber amplifier and up-conversion fiber lasers. In this paper, the mechanism and the progress of study on rare earth ions doped multi-component glass fibers in broad band fiber amplifier and up-conversion fiber lasers are introduced and reviewed. The questions and the applications of rare earth ions doped multi-component glass fibers in the future are also prospected. Based on the present research progress, it is suggested to further study the tellurite and bismuth glasses, which are used as fiber materials in broad band fiber amplifier. To up-conversion fiber laser, it is still need to further investigate novel glasses, which has low phonon energy and good physical and chemical properties.}

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2.0 μm spectroscopic properties of Er3+/Tm3+/Ho3+ triply-doped fluorophosphate glasses pumped by 808 nm and the energy transfer mechanisms between the three rare earth ions were investigated. J-O theory was used to calculate the parameters of Ho3+ in fluorophosphate glasses. Absorption and emission cross-sections and the gain coefficients were calculated. The obtained lifetime r and spontaneous transition probability Ar of Ho3+:5I7 level were 10.64 ms and 93.95 s-1 respectively. The calculated maximum emission cross-section of 2.0 μm was 9.26×10-21 cm2. The energy transfer analysis indicated that the cross-relaxation of Tm3+ was important and the resonent energy transfer in Er3+&rarrHo3+, Tm3+&rarrHo3+, Er3+&rarrTm3+&rarrHo3+ process was the main channel. The study revealed that the Er3+/Tm3+/Ho3+ triply-doped fluorophosphate glass would be a potential material for 2.0 μm emission because of the efficient sensitization of Er3+ and Tm3+ to Ho3+.

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Er3+-doped halide modified tellurite glasses were synthesized by conventional melting and quenching method. The Judd-Ofelt analysis was performed on the absorption spectra and the transition probabilities, excited state lifetimes, and the branching ratios were calculated and discussed. The intense infrared and visible fluorescence spectra under 980 nm excitation were obtained. Strong upconversion signal was observed at pumping power as low as 30 mW in the glasses with halide ions. The upconversion mechanisms and power dependent intensities were discussed, which showed two-photon process are involved for the green and red emissions. The decay times of the emitting states and the corresponding quantum efficiency were determined and explained. (C) 2004 American Institute of Physics.

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Er3+ -doped strontium lead bismuth glass for developing upconversion lasers has been fabricated and characterized. The Judd-Ofelt intensity parameters Omega(1) (t = 2,4,6), calculated based on the experimental absorption spectrum and Judd-Ofelt theory, were found to be Omega(2) = 2.95 x 10(-20), Omega(4) = 0-91 X 10(-20), and Omega(6) = 0.36 x 10(-20) cm(2). Under 975 nm excitation, intense green and red emissions centered at 525, 546, and 657 nm, corresponding to the transitions H-2(11/2) --> I-4(15/2), S-4(3/2) I-4(15/2), and F-4(9/2) --> I-4(15/2) respectively were observed. The upconversion mechanisms are discussed based oil the energy matching and quadratic dependence on excitation power, and the dominant mechanisms are excited state absorption and energy transfer upconversion for the green and red emissions. The long-lived I-4(11/2) level is supposed to serve as the intermediate state responsible for the upconversion processes. (C) 2004 Published by Elsevier B.V.

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Yb3+/ Er3+-codoped oxychloride germanate glasses have been synthesized by a conventional melting and quenching method. Structural properties were obtained based on Raman-spectra investigation, indicating that PbCl2 plays an important role in the formation of the glass network and has an important influence on the phonon density and the maximum phonon energy. The Judd - Ofelt intensity parameters and quantum efficiencies were calculated based on the Judd - Ofelt theory and lifetime measurements. The enhanced upconversion luminescence intensity of Er3+ with increasing PbCl2 content could not be explained only by the maximum phonon-energy change of the host glasses. For the first time, the effect of PbCl2 addition on phonon density, OH- content, and upconversion luminescence in oxychloride glasses has been discussed and evaluated. The results show that the effect of phonon density and OH- content on upconversion luminescence in oxychloride glasses is much stronger than that of the decrease of the maximum phonon energy. The possible upconversion luminescence mechanisms have also been estimated and are discussed.

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Three kinds of Er3+-doped tellurite glasses with different hydroxyl groups are prepared by the conventional melt-quenching method. Infrared spectra are measured to estimate the exact content of OH- groups in samples. The maximum phonon energy in glasses are obtained by measuring the Raman scattering spectra. The strength parameters Omega(t) (t = 2, 4, 6) for all the samples are calculated and compared. The nonradiative decay rate of the Er3+ I-4(13/2) -> I-4(15/2) transition are calculated for the glass samples with different phonon energy and OH- group contents. Finally, the effect of OH- groups on fluorescence decay rate of Er3+ is analysed, the constant KOH-Er Of TWN, TZPL and TZL glasses are calculated to be 9.2 x 10(-19) cm(4)s(-1), 5.9 x 10(-19) cm(4)s(-1), and 3.5 x 10(-19) cm(4)s(-1), respectively.

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Because of the influence of OH groups in phosphate glasses on the radiation of rare-earth ions, the laser performance is degraded. The laser efficiency and the small signal gain experiment of several phosphate glass samples have been done, the concentration of OH groups in glasses was calculated from the measured absorption coefficient at 3.47 μm. It is shown that the concentration of OH groups in phosphate glasses can seriously influence the laser output characteristics, and the OH groups have worse influence on the laser amplifier than laser oscillator.

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We report spectral properties and thermal stability of Nd3+-doped InF3-based heavy-metal fluoride glasses. Fluoroindate glasses in the chemical compositions (in mol%) of (38-x)InF3-16BaF(2)-20ZnF(2)-20SrF(2)-3GdF(3)-1GaF(3-)2NaF-xNdF(3) (x = 0.1, 0.5, 1, 2, 3) have been prepared under a controlled atmosphere in a dry box. Strong UVblue upconversion emission from a green excitation wavelength has been observed and the involved mechanisms have been explained. Near-infrared emission occurs simultaneously upon excitation of the UV-blue upconversion emissions with a cw Ar(+)laser. The upconversion spectra have revealed four dominant emissions at 354, 380, 412 and 449 nm, which belong to the transitions of D-4(3/2) -> I-4(9/2), D-4(3/2) -> I-4(11/2) and P-2(3/2) -> I-4(9/2), D-4(3/2) -> I-4(13/2) and P-2(3/2) -> I-4(11/2), D-4(3/2) -> I-4(15/2) and P-2(3/2) -> I-4(13/2), respectively.

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This paper reports on the optical spectroscopic properties and thermal stability of Er3+-doped TeO2-BaO (Li2O,NaO)-La2O3 glasses for developing 1.5-mu m fiber amplifiers. Upon excitation at 977 nm laser diode, an intense 1.53-mu m infrared fluorescence has been observed with a broad full width at half maximum (FWHM) of about 60 nm for the Er3+-doped TeO2-BaO (Li2O, Na2O)-La2O3 glass with 10 mol% of BaO. The calculated fluorescence lifetime and the emission cross-sections of the 1.53-mu m transition are 2.91 ms and similar to 9.97 x 10(-21) cm(2), respectively. It is noted that the gain bandwidth, a, x FWHM, of the TeO2-BaO-La2O3Er2O3 glass is about 600, which is significantly higher than that in silicate and phosphate glasses. Meanwhile, it is interesting to note that the TeO2-BaO-La2O3-Er2O3 glass has shown a high glass thermal stability and good infrared transmittance. As a result, TeO2-BaO (Li2O, Na2O)-La2O3 glass with 10 mol% of BaO has been considered to be more useful as a host for broadband optical fiber amplifier. (c) 2005 Elsevier B.V. All rights reserved.

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Intense room-temperature near infrared (NIR) photoluminescence (980 nm and 1032 nm) is observed from Yb,Al co-implanted SiO2 films on silicon. The optical transitions occur between the F-2(5/2) and F-2(7/2) levels of Yb3+ in SiO2. The additional Al-implantation into SiO2 films can effectively improve the concentration quenching effect of Yb3+ in SiO2. Photoluminescence exitation sprectroscopy shows that the NIR photoluminescence is due to the non-radiative energy transfer from Al-implantation-induced non-bridging oxygen hole defects in SiO2 to Yb3+ in the Yb-related luminescent complexes. It is believed that the defect-mediated luminscence of rare-earth ions in SiO2 is very effective.

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稀土元素由于在农业上的广泛应用已经越来越多地进入到生物体循环中,因此在分子水平上研究它们对生物体功能的影响及其作用机理成为人们迫切需要解决的课题。钙调蛋白(CaM)是广泛存在于生物体内的一种多功能的调节蛋白,调节着至少40余种酶的活性。基于上述原因,本文选取钙调蛋白作为研究对象,系统地比较了不同浓度的钙离子和稀土离子对它的靶酶钙调神经磷酸酶、磷脂酶凡、乳酸脱氢酶活性的影响,并采用荧光光谱、同步荧光光谱、紫外差谱、红外光谱等方法研究了它们对钙调蛋白及其靶酶构象变化的影响。发现稀土离子对钙调蛋白靶酶的活性均表现出"低浓度促进,高浓度抑制"的Hormesis效应,由于靶酶分子结构的差异,其最大激活浓度有所区别,钙调蛋白可以缓解稀土离子对靶酶的抑制作用;发现高浓度的稀土离子与钙调蛋白作用后,可以降低钙调蛋白与靶肤/酶分子的亲合性,并抑制其调节靶酶活性功能的发挥;稀土离子与钙调蛋白作用后,增大其α-螺旋含量,减少价折叠结构,对小肤的二级结构影响较小;二乙三氨五乙酸及其衍生物二乙三胺五乙酸-双二甲酞胺和二乙三胺五乙酸一双(异烟麟)可以作为乳酸脱氢酶的竞争性抑制剂抑制其活性,抑制常数分别为3.37、7.41、8.52μmol几,钙调蛋白也可以缓解它们对脱氢酶的抑制作用;首次制备出一株由稀土离子诱导钙调蛋白构象变化后的单克隆抗体2C3,该抗体可以特异性地识别含稀土的钙调蛋白,与Ca-CaM、La-CaM、Eu-CaM以及Yb-CaM之间的解离常数分别为157、26.8、21.8和64.8 nmol/L,该抗体还能够区分钙调蛋白结合不同浓度稀土离子后的构象状态。

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PDP(等离子平板显示器)是一种最有前途的大屏幕壁挂式彩电,而它需要VUV激发下的高效荧光粉,同时由于VUV荧光粉也是无汞荧光灯的需求,所以研究VUV激发的稀土激活的荧光粉是实际应用的需要.对于光谱分析该工作采用了理论计算与光谱数据分析相结合的方法,对所测光谱各个谱峰进行了详细的指认.得到了以下的结论和成果:1.得到了大量的含氧酸盐中稀土离子的VUV光谱数据.2.首次系统地应用两种方法预测了三价稀土离子的f-d跃迁位置,并首次系统地通过计算预测了三价稀土离子在含氧酸盐中的电荷迁移带的位置.3.首次实验观察到Ce<'3+>的电荷迁移带,观察到了Tb<'3+>的电荷迁移带.4.在所有含Dy<'3+>的样品中都观察到Dy<'3+>的f-d跃迁.5.LaPO<,4>和ABLa(PO<,4>)<,2>(A=K,Na;B=Mg,Zn)基质中,观察到了Ce<'3+>的5个f-d跃迁,指认了Tb<'3+>的5个f-d跃迁,指认了掺杂Ce、Tb的VUV光谱中的所有谱峰.6.对所研究基质中的稀土离子的f-d跃迁和电荷迁移带进行了系统地预测和指认.7.通过总结不同稀土离子在相同基质中的VUV光谱,并参考文献的相关报导,总结了所研究基质的基质吸收位置.8.通过Eu<'3+>的灾光探针作用和ce<'3+>的发射光谱等,确证三价稀土离子在La<,2>CaB<,10>O<,19>基质中同时取代了八配位的Ca<'2+>和十配位的La<'3+>,占据了两种格位.9.合成了一种新型绿色长余辉材料,具有亮度高,余辉时间长,可用日光激发等优点.10.合成了一种UV激发下性能优异的掺Eu<'3+>的红色荧光粉,亮度可以跟商业红粉Y<,2>O<,3>:Eu相比拟,而基质材料与Y<,2>O<,3>相比降低了成本.

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本论文通过水热、溶剂热、高温固相以及单晶生长法合成了复合氟化物及部分稀土离子激活的氧化物。运用近年来兴起的温和水热和溶剂热法探索了MAIF5(M=Ca、Sr、Ba)和LIMAIFa(M=Ca、Sr)系列复合氟化物的合成条件。以水作为溶剂,合成了CaAIF、SrAIF、BaA作ICaAIF6和L诏rAI凡化合物,从起始反应物、反应温度、反应时间及酸度儿方面考察了几种化合物的合成条件。对于溶剂热反应,选择了五种不同的溶剂作为反应介质,分别为乙二醇、乙醇、甲苯、毗咙、四氢「臾喃。以乙二醇和甲苯为溶剂,可以合成SrAlF5和LiSrAlF6民复合氟化物,而乙醇、毗咙、四氢「归喃作为反应介质没有得到l;l标产物。在五种汽半剂中均不能合成CoAIF6、BaAlF5和LiCaAlF6复合氟化物。通过水热、高温固相以及单晶生民法介成了KMgF3:Eu体系。水热合成的产,物具有氧含员低、物相纯等优点,同时该伙合成的多移,体存在史多的色心。比较三种方法合成的KMgFa:EU的光谱,发现水热和单晶样品中除了6P7/2→8S7/2的线发则外,还明显出现址火峰位置位于420nm处的带发射。结合退火实验,相刃刁又热样品的带发射是由于色心所致,而单晶样l界,的带峰则源于晶体中存在的色心、和少量氧所致,但以色心为主。在高温样品中,只有特征的线发射,没有观察到类似的带发射。结合退火前后线带发射弧度的变化及色心激发谱和翻”.6P7/2-8S7/2发射潜的乘补程度,得出Eu3+→色心的能址传递。通过高温固相反应合成Gd,Eu单掺、双掺的KMgFa、BaLiF3、BaY2F8三种磷光体,考察了Gd2+,Eu2+的光学性质,发现了双掺体系中(Gd3+→Eu2+的能里传递以生象,分析了能墩传递方式,并计算了前两个体系中Gd3+→Eu2+能最传递儿率。考察了Pr内+ 在KMgF2、LiYF4、BaY2F8基质中的光谱情况,指认了发射峰所对应的跃迁光潜项,具体讨论了KMgFa:Pr3+激发潜中352nm处的宽带激发峰。考察了Pr3+的发射弧度在KMg1-xCaxF3体系中的咨隋况,发现随枷含嫩的增加,Pr3+的在各发射区的发射强度显著增弧,分析了可能的原因。此外本论文也通过旋转试域熔融法生长了Ca2MgSi2O2单晶,详细讨论了生长品体的彩响因索,并以该化合物为纂质,考察了Eu的掺杂行为。在空气氛围下,没有发生Eu3+→Eu2+的还原,而是形成Ca2Eu8Si6O26化合物,这借助X-ray粉末衍射、组分分析及光谱分析得到证实。