Yb3+和Ce3+对Er3+掺杂碲酸盐玻璃光谱性质的影响

;在掺Er3 的70TeO2-20ZnO-5La2O3-5Nb2O5(各组成以摩尔比计)玻璃中引入Yb3 和Ce3 ,分析比较了975nm泵浦下Yb3 和Ce3 对于Er3 的1.5μm波段红外荧光和可见上转换发光特性的影响.结果表明:在掺Er3 的碲酸盐玻璃中引入Yb3 ,有效地提高了Er3 的1.5μm波段红外荧光强度、展宽了其荧光谱,也显著增强了可见上转换发光强度.随着玻璃中Ce3 的引入,进一步提高了Er3 的4I11/2→4I13/2能级间无辐射弛豫速率,1.5μm波段红外荧光也得到进一步增强,但可见上转换发光大幅减弱.与Er3 /Yb3 共掺相比,Er3 /yb3 /Ce3 共掺碲酸盐玻璃是一种更为理想的应用于1.5 μm波段宽带放大器的增益介质.     

二氧化硅对铒/铈共掺碲酸盐玻璃光谱性质的影响(英文)

为进一步提高Er3+1.53μm波段的光谱特性,在Er3+:4 I11/2→4 I13/2和Ce3+:2 F5/2→2 F7/2跃迁间存在能量失配(1 400cm-1附近)的Er3+/Ce3+共掺碲酸盐(TeO2-Bi2O3-TiO2)玻璃中引入了高声子能量SiO2组分。测试分析了不同SiO2组分含量下的Er3+吸收光谱、上转换发光谱、1.53μm波段荧光谱、荧光寿命、放大品质因子和玻璃样品的热性能。结果表明:由于增强的Er3+/Ce3+离子间能量传递,当玻璃样品中SiO2含量达到9%(摩尔分数)时,Er3+的1.53μm波段荧光强度得到显著提高。同时,荧光半高宽随SiO2组分含量相应展宽,而玻璃热稳定性随之提高。     

Yb~(3+)/Ho~(3+)共掺Ge_(25)Ga_5S_(70)玻璃中红外发光特性

用熔融急冷法制备了系列Yb3+/Ho3+共掺Ge25Ga5S70硫系玻璃,测试了样品的吸收光谱以及980nm激光泵浦下中红外荧光光谱特性,用Judd–Ofelt理论计算分析了单掺Ho3+在Ge25Ga5S70玻璃中的强度参数Ωi(i=2,4,6)、自发辐射跃迁几率、荧光分支比和辐射寿命等光谱参数。研究了Yb3+/Ho3+共掺样品在980nm激光泵浦下获得的Ho3+:2.9μm中红外荧光光谱性质,表明Yb3+/Ho3+之间存在能量共振转移。当固定Yb3+掺杂浓度为0.5%(质量分数,下同),随着Ho3+掺杂浓度从0增加为0.7%,Yb3+:2F5/2能级寿命明显单调下降,说明Yb3+/Ho3+之间有效的能量传递主要来源于Yb3+:2F5/2能级向Ho3+:5I6能级的共振能量传递。运用Futchbauer-Ladenburg公式计算比较了不同掺杂浓度下Ho3+:5I6→5I7跃迁的受激发射截面。     

金属离子掺杂对TiO_2:Yb~(3+)/Er~(3+)上转换材料发光性能的调控研究

稀土文章采用水热法合成掺杂不同金属离子的Ti O2:Yb3+/Er3+上转换发光材料。系统的探讨了不同的金属离子对Ti O2:Yb3+/Er3+发光材料发光性能、形貌以及晶型的影响。具体到通过荧光光谱数据分析离子价态、离子半径等对红、绿光性能的影响;通过SEM数据分析掺杂不同金属离子对应样品形貌的变化;通过XRD数据分析掺杂不同金属离子对应样品的晶型的变化。结果表明离子价态以及离子半径都会改变Ti O2:Yb3+/Er3+材料的发光性能,但与Ti O2:Yb3+/Er3+材料发光性能之间不存在线性关系;掺杂不同金属离子不会改变样品的形貌;掺杂不同金属离子得到了纯相的Ti O2:Yb3+/Er3+样品,且不改变样品的晶型。     

Tm3+/Ho3+共掺硫系玻璃光纤放大器增益特性

中红外2.0～3.5μm 波段激光在医疗、空气污染监测和军事等领域有着重要的应用前景。采用真空熔融淬冷法制备了 Tm3+/Ho3+共掺的Ge20Ga5Sb10S65硫系玻璃,测试了样品的吸收光谱以及800 nm激光泵浦下的荧光光谱,通过Judd–Ofelt和Mc-Cumber理论计算了Tm3+/Ho3+的辐射寿命、自发辐射几率和受激发射截面等光谱参数。在此基础上,研究了双掺离子之间的能量传递和Tm3+–Ho3+的多种跃迁过程,给出了详细的4能级系统的速率方程,并结合光功率传输方程,得出Tm3+/Ho3+共掺硫系玻璃光纤放大器在2μm波段的增益特性。数值模拟结果表明：Tm3+/Ho3+共掺硫系玻璃光纤在2μm波段的增益值达27 dB,增益带宽为112 nm,最佳掺杂光纤长度L=300 cm,所需泵浦功率Pp=200 mW,可用于2μm波段宽带放大。     

Influence of Microstructure Modulation of Er~（3＋）-Doped Al_2O_3 on the Photoluminescence Performance

采用溶胶–凝胶法分别制备了掺不同摩尔分数Er3＋的Er3＋：Al2O3粉末和不同摩尔分数Y3＋的0.5%Er3＋：Al2O3（Y3＋：0.5%Er3＋：Al2O3）粉末。利用Y3＋与Al3＋的半径差异,通过共掺不同掺量的Y3＋来调制Al2O3的微结构,用X射线衍射和透射电子显微镜分析样品的结构特征,并通过光致发光光谱研究样品的光致发光特性。结果表明：不同Y3＋和Er3＋共掺杂的Y3＋：Er3＋：Al2O3样品均以-Al2O3为主相;随着Y3＋掺量的增加,Al2O3的晶格缺陷逐渐增多;样品的荧光强度、发射谱宽度及荧光寿命也都随着Y3＋掺量增大而增大。通过Y3＋掺量调制Er3＋所处微结构环境的方法有效地改善了Er3＋：Al2O3材料的发光特性。     

敏化剂离子对Tm~(3+)掺杂的镓锗玻璃1.47-μm发光特性研究

报道了Tm3+掺杂的15Ga2O3-75Ge O2-10Na2O玻璃1.47-μm发光,应用Judd-Ofelt理论计算了玻璃的强度参数t(t=2,4,6)、自发辐射几率A、荧光分之比β等各项光谱参数以及峰值发射截面σepeak。通过测量光谱性能研究了敏化剂离子(Ho3+,Tb3+,Sm3+,Dy3+)掺杂浓度对Tm3+离子1.47-μm波段发光性能的影响,分析了Tm3+和这些敏化剂离子之间的能量传递过程。研究表明镓锗钠玻璃是适用于S波段光纤放大器的一种潜在基质材料,而掺杂一定浓度的敏化剂离子迅速降低了Tm3+:3F4能级的粒子数,而对3H4能级粒子数影响不大,极大地提高了Tm3+离子在1.47-μm波段的发光效率,且Tb3+是最有效的敏化剂离子。     

Er3+,Er3+-Yb3+和Er3+-Na+掺杂CaF2透明陶瓷的光学性能（英文）

以Ca(NO3)2、Er(NO3)3、Yb(NO3)3、KF和NaF为原料,采用热压烧结方法制备出Er3+,Er3+-Yb3+和Er3+-Na+掺杂CaF2透明陶瓷。测试了样品室温吸收光谱和发射光谱。利用Judd–Ofelt理论分析了样品的光学性能,并对吸收光谱进行计算拟合,得到光谱参数t(t=2,4,6),根据光谱参数t计算出Er3+某些能级的的跃迁几率、荧光分支比、辐射寿命和品质因子,讨论并比较了Er3+-Yb3+和Er3+-Na+共掺对CaF2透明陶瓷光学性能的影响。结果表明:掺杂Yb3+和Na+改变了Er3+光谱参数;Er3+-Yb3+共掺有利于提高样品的荧光强度;Er3+-Na+共掺有利于提高荧光寿命。     

In∶Yb∶Er∶LiNbO_3晶体的生长和光谱性能

采用提拉法生长了掺0.25%(摩尔分数,下同)Yb2O3,0.25%Er2O3和(0.5%、1.0%、1.5%)In2O3的3种同成分In∶Yb∶Er∶LiNbO3晶体。通过晶体的红外光谱,解释了In3+,Yb3+和Er3+在晶体中的占位,由于Yb3+和Er3+离子的掺入,在In∶Yb∶Er∶LiNbO3晶体中In3+既占据Li位又部分占据Nb位,使2%In∶Yb∶Er∶LiNbO3晶体达到阈值浓度。采用980nm二极管激光器测试了In∶Yb∶Er∶LiNbO3晶体上转换发射光谱。结果表明:晶体的绿光上转换发射中心波段位于525、550nm处,分别相应于Er3+的2 H11/2→4 I15/2跃迁和4 S3/2→4 I15/2跃迁;上转换红光发射中心波段在660nm处,对应Er3+的4 F9/2→4 I15/2辐射跃迁。In3+能提高Yb∶Er∶LiNbO3晶体的抗光损伤能力,改变Er3+和Yb3+的局部环境及Yb3+对Er3+的敏化作用,使得In∶Yb∶Er∶LiNbO3晶体发光性能改变。     

掺铒钨碲酸盐玻璃光谱性质的研究

研究了掺铒钨碲酸盐玻璃的吸收光谱和荧光光谱。应用JuddOfelt理论计算了Er3+的光谱强度参数Ωt(t=2,4,6)、自发辐射跃迁几率、荧光分支比和辐射寿命。从光谱强度参数的计算说明掺铒钨碲酸盐玻璃中Er—O键的共价性强于碲酸盐玻璃中Er—O键的共价性。玻璃的荧光半高宽为52nm,大于Er3+在磷酸盐和硅酸盐玻璃中的荧光半高宽。应用McCumber理论,计算了钨碲酸盐玻璃中Er3+离子在峰值波长1532nm的受激发射截面,为0.91×10-20cm2,大于Er3+在碲酸盐玻璃中的受激发射截面0.75×10-20cm2。由于掺铒钨碲酸盐玻璃的玻璃转变温度高、有较大的声子能量、较宽的荧光半高宽和较大的受激发射截面,是制作高增益的光波导放大器的理想材料。     

铒/镱共掺硼酸钙镧晶体的生长和光谱性质

在CaO-Li2O-B2O3助熔体系中,生长了掺铒和镱的硼酸钙镧(Er3 :Yb3 :La2CaB10O19,Er:Yb:LCB)晶体.Er:Yb:LCB晶体中Er3 ,Yb3 的分凝系数分别为0.50,0.25.X射线衍射分析表明:Er:Yb:LCB和LCB具有相同的晶体结构.Er:Yb:LCB晶体的熔点大约为1046℃.Er:Yb:LCB晶体的吸收光谱和荧光光谱的测试结果表明:与Er:LCB相比,Er:Yb:LCB晶体在970 nm的吸收系数显著提高,在1 531 nm的发射强度也显著增强,其荧光寿命为0.48 ms.     

2.0 μm Emission Properties and Energy Transfer between Ho3+ and Tm3+ in PbO—Bi2O3—Ga2O3 Glasses

Emission properties of 2.0 μm fluorescence and the energy transfer between Ho³⁺ and Tm³⁺ in 57PbO·25Bi₂O₃·18Ga₂O₃ (mol%) glass codoped with Ho³⁺ and Tm³⁺ were investigated. Cross-relaxation rates in Tm³⁺ increased approximately 5 times when the Tm₂O₃ concentration was increased from 1.0 to 1.5 wt%. Coefficients of the forward Tm³⁺→ Ho³⁺ energy transfer were about 15 times larger than those of the Tm³⁺← Ho³⁺ backward transfer. Analysis of the energy transfer and gain spectra indicated that the highest gain at the 2.0 μm wavelength region could be achieved from the glass with 1.5 wt% of Tm₂O₃ and 0.3 wt% of Ho₂O₃.     

Er~(3+)-Tm~(3+)共掺碲酸盐玻璃中近红外超宽带发光性质

研究了Er~(3+)-Tm~(3+)共掺TeO_2O-Nb_2O_5-Ln_2O_3(TKNL)碲酸盐玻璃的近红外发光光谱以及上转换光谱性质,该碲酸盐玻璃的起始析晶温度与玻璃转变温度之差△T为136℃,表明此玻璃具有良好的热稳定性,有利于拉制光纤。在808 nm半导体激光器的激发下在近红外波段观察到半高宽为185 nm的宽带近红外发光。通过对不同Tm~(3+)浓度以及不同激发波长下TKNL玻璃的近红外发光以及上转换发光的研究,探讨了Er~(3+)m~(3+)之间的能量传递机理。上述玻璃材料有望用作S和C波段光纤放大器的增益介质。     

Er3+掺杂TeO2-WO3-ZnO玻璃的发光性质

制备了不同组成和掺Er3 量的TeO2 WO3ZnO(TWZ)玻璃样品 ,测量了样品的吸收光谱和 970nmLD激发下的荧光光谱、荧光寿命。对制得的Er2 O3掺杂摩尔分数为 0 .6%的玻璃样品 ,由吸收光谱测得的 1.5 μm峰值吸收截面及计算的受激发射截面分别为 0 .74～0 .77pm2 和 0 .86～ 0 .90pm2 ,且玻璃的组成对其影响很小 ;Er3 在摩尔组成为 75TeO2 2 0WO35ZnO的TWZ玻璃中具有较大的荧光发射半高宽 (fullwidthathalfmaximum ,FWHM) ,且随掺Er3 量的增加 ,Er3 1.5 μm发射荧光强度和FWHM总体呈增加趋势 ,实验得到掺Er3 量为 3 .3 4× 10 2 0 /cm3时的FWHM为 80nm。研究同时发现Er3 在TWZ玻璃中具有很好的溶解性且其浓度猝灭效应较小     

Dazzling cool white light emission from Ce3+/Sm3+ activated LBZ glasses for W-LED applications

We synthesized a batch of co-doped (Ce³⁺+Sm³⁺): LBZ glass specimens by melt quenching process and their structural and radiation properties were studied by employing XRD, FE-SEM, optical absorption, photoluminescence and lifetime measurements. UV–Vis–NIR absorption studies of the co-doped (Ce³⁺+Sm³⁺): LBZ glassy matrix displays pertinent bands of both Ce³⁺ and Sm³⁺ ions. Individually doped Sm³⁺: LBZ glass exhibit bright orange emission at 603?nm (⁴G_5/2 → ⁶H_7/2) under the excitation of 403?nm. Nevertheless, the luminescence intensities pertaining to Sm³⁺ were extraordinarily increased by co-doping with Ce³⁺ ions to Sm³⁺: LBZ glassy matrices because of energy transfer from Ce³⁺ to Sm³⁺. The fluorescence spectra of co-doped (Ce³⁺+Sm³⁺): LBZ exhibits characteristic emission bands of Ce³⁺ (441?nm, blue) and Sm³⁺ (603?nm, reddish orange) under the excitation of 362?nm. Decay curves of Ce³⁺ and Sm³⁺ ions in co-doped glass has been fitted to double exponential nature. The decreasing lifetime of donor ion and rising lifetime of acceptor ion in double doped glass could support the energy transfer from Ce³⁺ to Sm³⁺ ions in the host matrix. The CIE coordinates and CCT values were calculated for all the obtained co-doped glassy samples from their luminescence spectra. By adding Ce³⁺ ions to individually doped Sm³⁺: LBZ glass matrix, the emitting color changes from reddish orange to white light which resembles the energy transfer from Ce³⁺ to Sm³⁺ ions. These studies, perhaps implied that attained co-doped (Ce³⁺+Sm³⁺): LBZ glassy samples are potential materials for white lighting appliances.     

Luminescence characteristics and energy transfer of Eu2+/Tb3+ doped single phase multi-color phosphor

The investigation on single phase multi-color phosphors is highly meaningful for near-ultraviolet chip based white light emitting diodes. In this work, a series of Eu²⁺ and Tb³⁺ singly doped and Eu²⁺/Tb³⁺ codoped Sr₅(PO₄)₃Cl phosphors were synthesized via a high-temperature solid state reaction method. The luminescence spectra and decay curves of Eu²⁺ and Tb³⁺ singly doped samples were discussed, the optimal doping concentrations were determined. Thanks to the spectra overlap between Eu²⁺ and Tb³⁺, nonradiative energy transfer from Eu²⁺ to Tb³⁺ was investigated. It is found electric dipole-dipole interaction played the main role for the energy transfer in codoped samples, the highest energy transfer efficiency was calculated to be 60.98%. Tunable emissions are observed for codoped samples by adjusting doping concentration. The thermal quenching properties were discussed and the activation energy (ΔE) was estimated in the present work.     

LaF3:Ce3+荧光特性的研究

LaF3：Ce多晶中Ce^3 的荧光发射谱由双峰带结构组成。Ce^3 与其他稀土粒子共掺杂，Ce^3 发射强度均降低，原因是一部分稀土离子(如Eu^3 等)与Ce^3 产生了电子转移；一部分稀土离子(如Er^3 等)与Ce^3 产生了能量传递。     

Color-tunable up-conversion luminescence of Zn(AlxGa1-x)2O4:Yb3+,Tm3+,Er3+ powders

Color-tunable up-conversion powder phosphors Zn(Al_xGa_1-x)₂O₄: Yb³⁺,Tm³⁺,Er³⁺ were synthesized via high temperature solid-state reaction. Also, the morphological and structural characterization, up-conversion luminescent properties were all investigated in this paper. In brief, under the excitation of a 980?nm laser, all powders have same emission peaks containing blue emission at 477?nm (attributed to ¹G₄→³H₆ transition of Tm³⁺ ions), green emission at 526?nm and 549?nm (attributed to ²H_11/2→ ⁴I_15/2 and ⁴S_3/2→⁴I_15/2 transition of Er³⁺ ions respectively), red emission at about 659?nm and 694?nm (attributed to ⁴F_9/2→⁴I_15/2 transition of Er³⁺ ions and ³F₃→³H₆ transition of Tm³⁺ ions, respectively), which are not changed after the doping of Al³⁺ ions. However, the doping of Al³⁺ ions can enhance the up-conversion luminescent intensity and efficiency, while the emission color of as-prepared powder phosphors can be tunable by controlling the doping amount of Al³⁺ ions. Taking Zn(Al_0.5Ga_0.5)₂O₄:Yb,Tm,Er as the cut-off value, the emissions have clear blue-shift firstly and then show obvious red-shift with the increasing doping of Al³⁺ ions. Stated thus, pink emission in ZnAl₂O₄:Yb,Tm,Er, purplish pink emission in ZnGa₂O₄:Yb,Tm,Er and Zn(Al_0.9Ga_0.1)₂O₄:Yb,Tm,Er, purple emission in Zn(Al_0.1Ga_0.9)₂O₄:Yb,Tm,Er and Zn(Al_0.3Ga_0.7)₂O₄:Yb,Tm,Er, purplish blue emission in Zn(Al_0.7Ga_0.3)₂O₄:Yb,Tm,Er, blue emission in Zn(Al_0.5Ga_0.5)₂O₄:Yb,Tm,Er can be observed, which confirm the potential applications of as-prepared Zn(Al_xGa_1-x)₂O₄:Yb³⁺,Tm³⁺,Er³⁺ powder phosphors in luminous paint, infrared detection and so on.     

Energy Transfer and Population Inversion in Heavy Metal Oxide Glasses Doped with Tm3+ and Tb3+

Emission properties and energy transfer of PbO–Bi₂O₃–Ga₂O₃–GeO₂ glasses codoped with Tm³⁺ and Tb³⁺ ions were investigated. The 1.48-μm emission due to the Tm³⁺:³H₄→³F₄ transition can be used to amplify the S-band (1460–1530-nm) signal light. With Tb³⁺ addition, the lifetime and emission intensity of the Tm³⁺:³F₄ level decreased sharply via the Tm³⁺:³F₄→Tb³⁺:⁷F_0,1,2 energy transfer. Population densities of the ³F₄ and ³H₄ levels in Tm³⁺ calculated from rate equations clearly verified that population inversion in Tm³⁺ ions became possible with as little as 0.1 mol% of Tb³⁺ addition.     

Color tunable Ba3Lu(PO4)3:Tb3+,Mn2+ phosphor via Tb3+→Mn2+ energy transfer for white LEDs

Series of UV excited Ba₃Lu(PO₄)₃:Tb³⁺,Mn²⁺ phosphors with tunable green to red emissions had been prepared using solid state reactions. Powder X-ray diffraction and Rietveld structure refinement were used to investigate the phase purity and crystal structure of the prepared samples. Under UV excitation, the Ba₃Lu(PO₄)₃:Tb³⁺,Mn²⁺ samples exhibited not only the typical Tb³⁺ emission peaks but also the broad emission band of Mn²⁺ ions due to the efficient Tb³⁺→Mn²⁺ energy transfer which had been verified by luminescence spectra and decay curves. Utilizing the Inokuti-Hirayama model, the Tb³⁺→Mn²⁺ energy transfer mechanism was determined to be the electronic dipole–quadrupole interaction. Moreover, the emission spectra of Ba₃Lu(PO₄)₃:0.80Tb³⁺,0.015Mn²⁺ sample at different temperatures manifested that our prepared phosphors possessed good thermal stability. The luminescence properties investigation results revealed the potential value of Ba₃Lu(PO₄)₃F:Tb³⁺,Mn²⁺ in application for UV excited phosphor converted white light emitting diodes.