SrF2晶体中Ho3+-Ho3+离子对的上转换发光研究

研究了在连续调谐以染料激光激发下,掺杂Ｈｏ＾３＋离子的ＳｒＦ２单晶中Ｈｏｌ＾３＋－Ｈｏ＾３＋对的上转换发光特性。Ｈｏ＾３＋－Ｈｏ＾３＋离子对的上转换发光主要分布于;强＾５Ｆ３→＾５Ｉ８跃迁４８０ｎｍ蓝色发射,较强＾５Ｓ２,＾５Ｆ４→＾５Ｉ８跃迁的５４０ｎｍ绿色发射。     

Eu^2＋和Mn^2＋在Sr3MgSi2O8中的光致发光研究

研究了Ｅｕ＾２＋和Ｍｎ＾２＋共激活的Ｓｒ３ＭｇＳｉ２Ｏ８的荧光性质。Ｅｕ＾２＋和Ｍｎ＾２＋在４６０ｎｍ和６９０ｎｍ的发射峰分别由Ｅｕ＾２＋的５ｄ→４ｆ跃迁和Ｍｎ＾２＋的＾４Ｔ１（＾４Ｇ）→＾６Ａ１ｇ（＾６Ｓ）跃迁产生。未观察到单掺杂Ｍｎ＾２＋的Ｓｒ３ＭｇＳｉ２Ｏ８的荧光发射，而掺入Ｅｕ＾２＋后则出现了Ｍｎ＾２＋的６９０ｎｍ光致发光峰，表明Ｅｕ＾２＋对Ｍｎ＾２＋有敏化作用。Ｅｕ＾２＋的荧光寿命也受Ｍ     

Ga3+对Ce3+光致发光的影响

研究了Ｇａ３＋在ＳｒＳ∶Ｃｅ和ＳｒＧａ２Ｓ４∶Ｃｅ薄膜电致发光（ＴＦＥＬ）材料中的作用及其对Ｃｅ３＋发光特性的影响。在ＳｒＳ中掺入Ｇａ２Ｓ３并烧结，发现Ｇａ３＋的浓度增加时，Ｃｅ３＋的发光显著向短波方向移动，激发谱中对应于ＳｒＳ带间吸收的激发峰相对减弱，而对应于Ｃｅ３＋的基态到激发态跃迁的激发效率相对提高，并出现逐渐增强的ＳｒＧａ２Ｓ４的带间吸收。Ｇａ３＋的引入使Ｃｅ３＋周围的配位场发生变化，相应的能级分布有所改变，Ｓｒ２＋离子性的增强和Ｃｅ３＋－Ｃｅ３＋相互作用的减弱对Ｃｅ３＋发光特性有显著影响。     

掺Eu3+离子Y2SiO5晶体格位选择光谱研究

分别利用白光灯、４５７－９ ｎｍ 氩离子激光、二倍频ＹＡＧ∶Ｎｄ 激光泵浦的诺丹明６Ｇ 可调谐窄线宽（０－５ ｃｍ －１） 染料激光作为光源， 以单色仪锁相放大器光电倍增管计算机数据采集系统记录光谱， 测量并研究了Ｙ２ＳｉＯ５∶Ｅｕ３ ＋ 晶体的透射光谱、荧光光谱、激发光谱和格位选择荧光光谱。５Ｄ０ →７Ｆ０，１ ，２ ，３，４ 跃迁，３０ 多根谱线（总数为５０ 根） 被观察到。在该晶体中Ｅｕ３＋ 替换Ｙ３＋ 离子， 占据两个较低对称性的光学格位， 这两个格位的５Ｄ０ ７Ｆ０ 能级跃迁谱线相隔大约只有０－２ ｎｍ ， 在室温下有一定的光谱关联。并用Ｘ射线谱对晶体的晶格常数ａ ， ｂ，ｃ 和晶面角度β进行测量， 测量结果显示掺杂后的晶格常数和未掺杂的Ｙ２ＳｉＯ５ 晶格常数基本一致。     

Eu^3＋,Bi^3＋Me2Y8（SiO4）6O2中的发光特性与取代格位

在紫外光激发下，Ｅｕ＾３＋和Ｂｉ＾３＋在Ｍｅ２Ｙ８（ＳｉＯ４）６Ｏ２基质（Ｍｅ＝Ｍｇ，Ｚｎ，Ｃａ，Ｓｒ）中分别发射红光（＾５Ｄ０－＾７Ｆ２）和蓝光（＾３Ｐ１－＾１Ｓ０）．Ｅｕ＾３＋发光的红橙比随着激发波长和Ｍｅ＾２＋的不同而变化。荧光拉曼光谱表明，Ｅｕ＾３＋在四种基质中同时占据了４ｆ格位和６ｈ格位。依据Ｂｉ＾３＋发光的Ｓｔｏｋｅｓ位移推断，当Ｍｅ＝Ｃａ，Ｚｎ时，Ｂｉ＾３＋主要占据４ｆ格位，而当Ｍｅ     

Eu^2＋和Mn^2＋在SrMgP2O7中的光致发光及其能量传递

研究了Ｅｕ＾２＋、Ｍｎ＾２＋共激活的ＳｒＭｇＰ２Ｏ７的发光性质、浓度与荧光性质的关系，Ｅｕ＾２＋和Ｍｎ＾２＋的发射光谱分别在４００ｎｍ及６７０ｎｍ附近，它们是Ｅｕ＾２＋的５ｄ－４ｆ跃迁和Ｍｎ＾２＋的＾４Ｔ１（＾４Ｇ）－＾６Ａ１ｇ（＾６Ｓ）跃迁发射，实验结果表明，Ｅｕ＾２＋对Ｍｎ＾２＋的荧光发射有较强的敏化作用，Ｍｎ＾２＋对Ｅｕ＾２＋的荧光寿命和强度也有显著影响。     

Eu2+在多相体系中的发光

研究了基质结构与离子半径的形成关系和Ｅｕ２＋在同时形成的多相体系中的发光现象．在ＭＭｇＡｌ１０Ｏ１７体系中,当Ｍ离子半径小于０．１０ｎｍ时,体系形成多相共存．首次观察到在磁铅矿、尖晶石和α－Ａｌ２Ｏ３三相同时共存体系中,Ｅｕ２＋优先占据离子半径和电荷与之匹配的磁铅矿中的Ｃａ２＋离子格位,不进入尖晶石和α－Ａｌ２Ｏ３晶相中的Ｍｇ２＋、Ａｌ３＋离子格位,仅产生Ｅｕ２＋的ｄ→ｆ跃迁宽带发射,且观察不到Ｅｕ３＋的特征光谱;在尖晶石和α－Ａｌ２Ｏ３两相同时共存体系中,Ｅｕ２＋可进入尖晶石和α－Ａｌ２Ｏ３晶相中的Ｍｇ２＋、Ａｌ３＋离子格位,分别产生Ｅｕ２＋的ｄ→ｆ和ｆ→ｆ跃迁发射,同时还观察到相当强的Ｅｕ３＋的特征光谱;在α－Ａｌ２Ｏ３单一相中,Ｅｕ２＋产生ｆ→ｆ跃迁发射,并观察到明显的Ｅｕ３＋的特征光谱,在α－Ａｌ２Ｏ３与γ－Ａｌ２Ｏ３同时存在的混合相中,Ｅｕ２＋的ｆ→ｆ跃迁发射消失,产生新的ｄ→ｆ跃迁宽带发射     

立方Gd2O3∶Eu纳米晶及光谱性质

用透射电镜拍摄球形ＣＧｄ２Ｏ３∶Ｅｕ纳米晶,并研究了室温下它的激发和发射光谱。结果表明,９００℃制备的体材料和相应的纳米晶相比,其激发光谱存在明显差异。前者以基质激发带为主导,电荷转移带（ＣＴＢ）很弱,而后者以ＣＴＢ为主。在绝缘体稀土氧化物中,可以忽略纳米效应对Ｅｕ３＋离子的４ｆ４ｆ能级跃迁的激发和发射光谱峰位的影响     

金属性Zintl相化合物RE_3Cu_3Sb_4(RE=Nd,Sm,Tb,Dy,Ho)的合成、结构及成键特性

用电弧熔炼方法合成了化合物ＲＥ３Ｃｕ３Ｓｂ４（ＲＥ＝ Ｎｄ,Ｓｍ ,Ｔｂ,Ｄｙ,Ｈｏ）, 采用粉末Ｘ射线衍射方法测定了其晶体结构。化合物属立方晶系,Ｙ３Ａｕ３Ｓｂ４ 类型, 空间群Ｉ４３ｄ（Ｎｏ．２２０）,皮尔森玛ｃＩ４０。晶胞参数：Ｎｄ３Ｃｕ３Ｓｂ４ ：ａ＝０．９６７４９（１） ｎｍ, Ｖ＝０．９０５６１（３） ｎｍ３;Ｓｍ３Ｃｕ３Ｓｂ４：ａ＝ －０．９６１４５（１） ｎｍ ,Ｖ＝０．８８８７５（３） ｎｍ３ ;Ｔｂ３Ｃｕ３Ｓｂ４： ａ＝０．９５３６２（１） ｎｍ , Ｖ＝ ０．８６７２１（３）ｎｍ３;Ｄｙ３Ｃｕ３Ｓｂ４： ａ＝０．９５０８８（１） ｎｍ , Ｖ＝０．８５９７５（３） ｎｍ３;Ｈｏ３Ｃｕ３Ｓｂ４ ： ａ＝０．９４８８（２） ｎｍ , Ｖ＝０．８５４１（５） ｎｍ３。每个单胞中包含４ 个化合式量。此结构中,Ｃｕ 原子均处于Ｓｂ 原子所形成的配位四面体中心, 这些共价结合的配位四面体通过共顶最终联接形成三维ＣｕＳｂ 网络,稀土原子则散布在网络之间的空隙中。化合物电荷平衡结构式可表示为ＲＥ３＋３ Ｃｕ１＋３ Ｓｂ３－４ , 化合物具有导电性, 为金属性Ｚｉｎｔｌ 相。原子成键具有典型过渡性。原子的“配位数”遵从配位环境规律。化合物的     

镧系离子与5,7-二氯-8-羟基喹啉-藏红花三元离子缔合物的萃取-光度分析特性

以Ｓｍ３＋为例研究了Ｌｎ３＋５，７二氯８羟基喹啉（ＤＣＯ）藏红花（ＳＦＴ）形成三元离子缔合物的萃取光度特征。用平衡移动法测定了离子缔合物的摩尔比Ｌｎ３＋∶ＤＣＯ∶ＳＦＴ＝１∶４∶１。在ｐＨ６８０～７５０的范围内，萃取物的λｍａｘ＝５２４ｎｍ，εｍａｘ＝４７０×１０４Ｌ·ｍｏｌ－１·ｃｍ－１。Ｓｍ３＋在０２～１５μｇ·ｍｌ－１范围内符合比尔定律。研究表明镧系离子的相对吸光度（ＡＬｎ／ＡＬａ）随原子序数呈现奇偶变化规律。     

Upconversion Properties of LiNbO_3 Single Crystals Co-doped with Ho and Yb

The IR-to-visible upconversion fluorescent crystals, Yb:Ho:LiNbO3, with a constant Ho3+ concentration (0.1 mol%) and different doping concentrations of Yb3+ (0.5, 1.5, 2.0, 2.5, 3.0 mol%) are synthesized by Czochralski method in air atmosphere. X-ray diffraction shows that the obtained crystal is a single phase of LiNbO3 and the rare-earth ions occupied the Li+ or Nb5+ sites instead of the interstitial sites. Under 980 nm excitation, green and red emission bands due to the Ho3+ (5S2, 5F4)/5I8 and Ho3+ 5F5/5I8 energy transitions are observed in these samples, respectively. Power dependence studies on these samples with different Yb3+ dopant concentrations indicate that the red and green emissions are based on a two-photon process. The intensities of the red and green upconversion fluorescence increase with Yb3+ ions of 0~2.0 mol% because of an increased Yb3+ sensitization, but decrease at higher concentrations owing to the back-energy transfer between the Yb3+ and Ho3+ ions.     

Effect of ZnX (X=F2 and Cl2) as modifier on luminescence properties of Ho3+/Yb3+ doped tellurite glasses

Optical absorption and photoluminescent properties of Ho(3+)/Yb(3+) co-doped tellurite and zinc halide tellurite glasses are investigated. The effect of zinc halides as modifier on the luminescence properties of above mentioned samples has been explored. Two intense upconversion emission bands centered at 546 ((5)F(4), (5)S(2)→(5)I(8)) and 660 ((5)F(5)→(5)I(8)) nm are observed when samples are excited by 976 nm radiation. Zinc halides act as quencher when 976 nm excitation source is used. The up and downconversion emission spectra are recorded with 532 nm excitation source also. In this case also, zinc halides do not show any improvement. The dependence of upconversion intensities on excitation power and temperature is discussed. The power dependence study shows a quadratic dependence of fluorescence intensity on the excitation power while decrement in emission intensity of different transitions at different rates is observed in temperature dependence study. The possible upconversion mechanisms are also discussed in order to understand the energy transfer between Yb(3+) and Ho(3+) ions.     

Fluorescence investigation of Ho3+ in Yb3+ sensitized mixed-alkali bismuth gallate glasses

Efficient 2.0 microm infrared and visible upconversion emissions have been observed in Ho3+/Yb3+ co-doped mixed-alkali bismuth gallate (LKBBG) glasses having a maximum-phonon energy of 673 cm(-1). The Judd-Ofelt parameters Omega2, Omega4 and Omega6 of Ho3+ indicate that there is a high asymmetry and strong covalent environment in LKBBG glasses. The large absorption and emission cross-sections of Yb3+ confirm that it is a suitable sensitizer for capturing and transferring pump energy to Ho3+. The emission cross-section profile for the 5I7-->5I8 transition is derived using the reciprocity method and the peak value is 5.54 x 10(-21)cm2, which is much larger than the value in fluorozircoaluminate glasses. LKBBG glasses exhibit low maximum-phonon energy and large refractive index, and it is possible to achieve an effective 1.66 microm U-band emission of Ho3+ under 900 nm laser radiation.     

Study of upconversion fluorescence property of novel Er3+/Yb3+ co-doped tellurite glasses

Er3+/Yb3+ co-doped TeO2-B2O3-Nb2O5-ZnO (TBN) glasses were prepared. The absorption spectra and upconversion luminescence spectra of TBN glasses were measured and analyzed. The upconversion emission bands centered at 530, 546 and 658 nm were observed under the excitation at 975 nm, corresponding to the transitions of 2H11/2-->4I15/2, 4S3/2-->4I15/2 and 4F9/2-->4I15/2 respectively. The ratio of red emission to green emission increases with an increasing of Yb3+ ions concentration. According to the quadratic dependence on excitation power, the possible upconversion mechanisms and processes were discussed.     

Upconversion and fluorescence spectral studies of Er3+/Yb3+-codoped Bi2Q3-GeO2-Ga2Q3-Na2O glasses

The absorption spectra and upconversion fluorescence spectra of Er3+/Yb3+-codoped natrium-gallium-germanium-bismuth glasses are measured and investigated. The intense green (533 and 549 nm) and red (672 nm) emission bands were simultaneously observed at room temperature. The quadratic dependence of the green and red emission on excitation power indicates that the two-photon absorption processes occur. The influence of Ga2C3 on upconversion intensity is investigated. The intensity of green emissions increases slowly with increasing Ga2O3 content, while the intensity of red emission increases significantly. The possible upconversion mechanisms for these glasses have also been discussed. The maximum phonon energy of the glasses determined based on the infrared (IR) spectral analysis is as low as 740 cm-1. The studies indicate that Bi2O3-GeO2-Ga2O3-Na2O glasses may be potential materials for developing upconversion optical devices.     

MgAl2O4∶Er^3+,Yb^3+荧光粉的制备及其上转换发光性能

以尿素为沉淀剂,采用低温水热法结合煅烧过程制备出MgAl2O4∶Er^3+,Yb^3+上转换荧光粉,并对样品的结构、微观形貌及上转换发光性能予以表征。结果表明,随尿素加入量的增大,产物主形貌由六角片状结构向纳米棒状转变,经1100℃煅烧可得纯相镁铝尖晶石结构,且Er^3+和Yb^3+能有效进入MgAl2O4晶格并占据Mg^2+位置形成均匀固溶体。在980 nm光激发下,MgAl2O4∶1.0%(n/n)Er^3+,x%(n/n)Yb^3+(x=0~8.0)荧光粉表现出在524、545 nm处绿光以及658 nm处的强红光发射,红绿光强度均在5.0%(n/n)Yb^3+掺杂时达到最大,但红绿光强度比却在7.0%(n/n)Yb^3+掺杂时达到最大值5.2,这归因于Er^3+-Er^3+之间交叉弛豫(CR)在红光发射过程中所起的重要作用。通过控制荧光粉中Yb^3+的掺杂量,能初步实现对于黄绿光色度的有效调控。     

Er~(3 )/Yb~(3 )共掺杂AlF_3基氟化物玻璃材料的频率上转换

Er3 /Yb3 共掺杂的AlF3基氟化物玻璃材料ABCY的制备及其上转换荧光性质。样品的组分为 40AlF3 2 0BaF2 2 0CaF2 (2 0 2x 2y)YF3 xEr2 O3 yYb2 O3。在 95 0nm连续LD激发下 ,观察到该材料很强的绿色上转换发光 ,研究了该体系的上转换机理 ,认为Yb3 和Er3 之间的APTE效应是最主要的上转换途径。解释了红、绿色上转换荧光强度比值增大的现象 ,指出了可能的交叉弛豫过程。用公式y =a(x -x0 ) n 对上转换荧光强度与LD工作电流的关系进行拟合 ,得到的结果与理论值很好地一致。     

Host dependent frequency upconversion of Er3+/Yb3+-codoped bismuth-germanate glasses

The absorption and upconversion fluorescence spectra of a series of Er3+/Yb3+-codoped xBi(2)O(3)-(90-x)GeO2-10Na(2)O (BGN x, x=31, 36, 41, 46 and 51 mol%) glasses have been studied. Intense green and red emission bands at around 533, 548 and 659 nm, corresponding to the 2H(11/2)-->4I(15/2), 4S(3/2)-->4I(15/2) and 4F(9/2)-->4I(15/2) transitions of Er3+, respectively, were simultaneously observed at room temperature. The dependence of intensities of upconversion emission on excitation power and possible upconversion mechanisms were evaluated and analyzed. The important role of Bi(2)O(3) in upconversion intensity is observed and its influence on the green (533 and 548 nm) and red (659 nm) emissions is compared and discussed. The influence of Bi(2)O(3) on the upconversion emissions has been investigated based on the IR spectra.     

Yb ion as a sensitizer for the upconversion luminescence in nanocrystalline Gd3Ga5O12:Ho

The effect of Yb³⁺ co-doping on the upconversion luminescence in nanocrystalline Gd₃Ga₅O₁₂:Ho³⁺ was examined. Strong and efficient NIR to green anti-Stokes luminescence was noted in nanocrystalline Gd₃Ga₅O₁₂:Ho³⁺, Yb³⁺ after excitation into the ²F_5/2 level of Yb³⁺ with 978 nm radiation. Weaker blue, red and NIR anti-Stokes luminescence was also observed after 978 nm excitation. An enhancement of the red ⁵F₅ → ⁵I₈ luminescence was observed in the anti-Stokes spectrum compared to the Stokes emission spectrum. This enhancement was attributed to two distinct energy transfer upconversion (ETU) mechanisms which preferentially populate the (⁵F₄, ⁵S₂) and ⁵F₅ levels.     

Green and red light emission by upconversion from the near-IR in Yb(3+) doped CsMnBr3

Direct near-IR excitation of Yb(3+) 2F(7/2)-->(2)F(5/2) levels at 10126, 10138, and 10596 cm(-1) in CsMnBr3:0.5%Yb(3+) leads to three types of luminescence at cryogenic temperatures: near-IR Yb(3+) emission and green and red upconverted luminescence. The green luminescence around 20 000 cm(-1) is identified as cooperative Yb(3+) pair upconversion. The broad red upconversion luminescence band centered at 14 700 cm(-1) is ascribed to the 4T(1g)-->6A(1g) transition of Mn(2+). Pulsed measurements indicate a sequence of ground-state absorption and excited-state absorption steps for the red upconversion process. One- and two-color excitation experiments support this, and we conclude that the red upconversion occurs by an exchange mechanism involving Yb(3+) and Mn(2+). The Yb(3+) 2F(5/2)-->(2)F(7/2) near-IR emission around 10 000 cm(-1) is also observed after Mn(2+) excitation at 21 838 cm(-1). This is indicative of a Mn(2+) 4T(1g)--> Yb(3+) 2F(5/2) relaxation process, which is a potential loss process for upconversion efficiency.