Pr￣（3＋）在SBN晶体中的发光特性

通过测量Ｐｒ：ＳＢＮ晶体的吸收光谱和荧光光谱来确定Ｐｒ￣（３＋）在ＳＢＮ晶体中的能级位置。由于Ｐｒ￣（３＋）离子占据晶体中的不同格位而引起荧光带呈现双峰结构。测量荧光寿命随温度的变化关系，表明Ｐｒ￣（３＋）在ＳＢＮ晶体中￣３Ｐ＿０态的无辐射弛豫主要是￣３Ｐ＿０→￣１Ｄ＿２多声子弛豫过程。     

Tm3+离子掺杂的钨酸钇钠晶体中浓度猝灭效应的研究

测量了Tm³⁺离子不同浓度(0.5at.%, 3 at.%, 5 at.%)掺杂的NaY(WO₄)₂晶体在800nm激光二极管激发下的上转换发射光谱.结合吸收谱、荧光谱和由Judd-Ofelt理论计算的光谱参数，详细分析了Tm³⁺:NaY(WO₄)₂晶体中上转换能量传递机理和离子浓度对上转换发射的影响.讨论了四种影响上转换发光效率的离子间相互作用机理：³H₅+¹G₄→³H₆+¹D₂，³H₅+³H₅→³H₆+³F₃，¹G₄+³H₆→³F₄+³F₃，¹G₄+³H₆→³F₃+³F₄，并根据Miyakawa-Dexter理论定量计算了各过程的发生概率.论证了交叉弛豫和共协上转换等浓度猝灭效应是影响Tm³⁺离子蓝色上转换荧光发射效率的主要因素. 关键词： 3+离子')" href="#">Tm³⁺离子 4)₂晶体')" href="#">NaY(WO₄)₂晶体 上转换 浓度猝灭     

Tm3+,Yb3+共掺ZBLAN玻璃中的能量传递与上转换

ＺＢＬＡＮ∶Ｔｍ³⁺，Ｙｂ³⁺玻璃在９７０ｎｍ二极管激光照射下发射明亮丰富的蓝、红上转换荧光．¹Ｇ₄和³Ｆ₄能级的发光是由Ｙｂ³⁺向Ｔｍ³⁺的逐步能量传递而来．而¹Ｄ_２能级发光是进一步由Ｔｍ³⁺离子之间的交叉能量传递而来．分析了Ｔｍ³⁺离子间的交 关键词：     

R1-xPrxBa2Cu3O7-δ超导Tc平台的离子尺寸效应

系统地研究了Ｒ_1-xＰｒ_xＢａ₂Ｃｕ₃Ｏ_7-δ的超导Ｔ_c与Ｐｒ替代浓度ｘ的关系。发现在离子半径ｒ_i≤ｒ_i（Ｄｙ）时，在低Ｐｒ浓度范围内存在一个超导Ｔ_c平台，并且平台宽度表明一个Ｒ^３＋离子尺寸效应。我们认为，Ｔ_c平台宽度的离子尺寸效应可能起源于Ｐｒ４ｆ电子局域态的改变。提出一个临界Ｒ^３＋离子半径ｒ_ic，ｒ_i＞ｒ_ic时ＲＢａ₂Ｃｕ₃Ｏ_7-δ的超导电性消失 关键词：     

NaLa(MoO4)2∶Eu3+的水热调控合成与发光特性研究

采用水热法合成了不同粒径的NaLa(MoO₄)₂∶Eu³⁺微晶.通过调节乙二醇浓度和反应时间,研究了NaLa(MoO₄)₂∶Eu³⁺微晶的形貌演变过程,在水热条件下180 ℃反应16 h获得了均一梭子形NaLa(MoO₄)₂∶Eu³⁺微晶,其晶粒长度约为2.0 μm.荧光光谱分析表明,Eu³⁺取代了NaLa(MoO₄)₂中La³⁺的格位, Eu³⁺在613 nm处红光发射(⁵D₀–⁷F₂跃迁)的浓度猝灭机理是电偶极-电四极相互作用,并发生了Eu³⁺( ⁵D₁ ) + Eu³⁺(⁷F₀ )→ Eu³⁺( ⁵D₀ ) + Eu³⁺(⁷F₃) 交叉弛豫,由此导致浓度猝灭. 关键词： 钼酸盐 水热法 稀土离子 发光     

调谐激光晶体Cr3+:ZnWO4光致发光特性的研究

研究了调谐激光晶体Ｃｒ³⁺：ＺｎＷＯ₄的光致发光特性。报道了它的吸收光谱、激发光谱、发射光谱及其随温度的变化、零声子跃迁和发射寿命等实验结果，并讨论了激发特性、电子－声子耦合作用、ＺｎＷＯ₄中Ｃｒ³⁺的发射寿命曲线等相关问题。 关键词：     

LnP5O14晶体中Tb3+和Eu3+的发光光谱特性

本工作测量了室温下TbP₃O₁₄和EuP₅O₁₄晶体的吸收和发射光谱。根据吸收光谱和Judd-Ofelt理论计算了Tb³⁺和Eu³⁺的实验和理论的振子强度。用最小二乘法拟合实验与理论的振子强度得到唯象强度参量Ω_λ。然后计算了Tb³⁺的⁵D₃→⁷F₅,⁵D₄→⁷F₄和⁵D₄→⁷F₆以及Eu³⁺的⁵D₀→⁷F₂,⁵D₀→⁷F₄的跃迁几率和寿命。同时用时间分辨光谱测量了不同温度下相应的荧光辐射寿命。计算与实验结果基本相符。理论和实验的结果表明Tb³⁺的⁵D₃态的寿命主要取决于⁵D₃→⁵D₄和⁷F₆→⁷F₀两能级对之间的电偶极-电偶极交叉弛豫。 关键词：     

CH2Br2的同步辐射光电离研究:10—12eV范围内CH2Br2的振动自电离态

报道在超声射流冷却条件下用同步辐射ＶＵＶ光源研究ＣＨ₂Ｂｒ₂的振动自电离结构．根据测量的１０５—１２３ｎｍ范围内母体离子（ＣＨ₂Ｂｒ₂⁺）的光电离产率曲线，获得ＣＨ₂Ｂｒ₂的绝热电离势为１０.２３±０.０１ｅＶ．ＣＨ₂Ｂｒ₂⁺的最低三个电子激发态，即Ａ（²Ａ₂），Ｂ（²Ｂ₁），Ｃ（²Ａ₁）分别位于１０.７８±０.０１ｅＶ，１１.２０±０.０１ｅＶ和１１.２７±０.０１ｅＶ．在１１５.０１—１２１.１５ｎｍ范围内，观察到ＣＨ₂Ｂｒ₂自电离峰叠加在若干台阶结构上，台阶平均宽度为７１６.８±４０.０ｃｍ^-1，对应于ＣＨ₂Ｂｒ₂⁺（Ｘ²Ｂ₂）中Ｂｒ-Ｃ-Ｂｒ反对称的伸缩振动（ｖ₉），所有的峰均归属为收敛于ＣＨ₂Ｂｒ₂⁺（Ｘ²Ｂ₂，ｖ⁺）振动能级的ｎｓ，ｎｐ和ｎｄ自电离Ｒｙｄｂｅｒｇ态．此外，对ＣＨ₂Ｂｒ₂光解离电离产生离子型自由基ＣＨ₂Ｂｒ⁺（Ｘ）的光电离产率曲线的结构也进行了归属 关键词：     

钌(Ⅱ)配合物与DNA相互作用的瞬态发光特性

以三种新合成的钌配合物[Ru(bpy)₂(7-CH₃-dppz)]²⁺、[Ru(bpy)₂(7-F-dppz)]²⁺、[Ru(phen)₂(7-F-dppz)]²⁺为研究对象,采用时间分辨的荧光光谱技术分别测量了这三种钌配合物与小牛胸腺DNA相互作用时的瞬态荧光动力学过程。结果表明:[Ru(bpy)₂(7-CH₃-dppz)]²⁺的发光寿命最长(约382 ns),而[Ru(bpy)₂(7-F-dppz)]²⁺的发光寿命最短(约65 ns)。分析表明:钌配合物的发光来源于配合物分子中的电荷转移态到基态的辐射跃迁。通过钌配合物与DNA的相互作用,使得配合物激发态分子的无辐射弛豫几率减小,从而导致发光寿命的增加。配合物的分子与DNA相互作用越强,激发态分子的无辐射弛豫几率越小,发光寿命也越长,最终导致高的发光效率。配合物的分子结构对配合物的分子与DNA的相互作用具有重要的影响。     

Ni2+:BeAl2O4晶体发光性质的研究

用时间分辨的激光诱导荧光光谱方法测量了10—300K温度范围内Ni²⁺:BeAl₂O₄晶体的红外荧光光谱和荧光寿命。通过荧光寿命的温度变化特性分析,得出³T_2g态的内禀辐射衰减寿命为123±7.2μs。无辐射弛豫的Mott激活能为1147cm^-1,并导出了此晶体发光量子效率随温度的变化关系式。Ni²⁺:BeAl₂O_{4关键词：}     

Spectroscopic properties of Pr:KY(MoO4)2 crystal as a visible laser gain medium

A Pr³⁺-doped KY(MoO₄)₂ single crystal was grown by the Czochralski method. The polarized absorption and fluorescence spectra of the Pr³⁺:KY(MoO₄)₂ crystal were measured at room temperature. The stimulated emission cross-sections for the transitions from the ³P₀ multiplet were estimated from the fluorescence spectra. The fluorescence lifetime of the ³P₀ multiplet was estimated from the fluorescence decay curve at room temperature. The analysis of spectral properties shows that the Pr³⁺:KY(MoO₄)₂ crystal is a promising gain medium for visible lasers.     

SBN晶体中Eu3+激发态的能量传递

通过选择激发SBN晶体中处于不同晶场位的Eu³⁺离子,得到⁵D₀→⁷F₁的时间分辨荧光光谱,确定了不等价晶场位的离子间的能量转移速率。荧光峰随激发波数的变化表明局部晶场的连续畸变。 关键词：     

Spectroscopic properties of Pr 3+ in anisotropic PbWO4 crystal

The polarized absorption spectra, polarized fluorescence spectra, and fluorescence decay curves of Pr³⁺ ions in anisotropic PbWO₄ single crystal, which was grown by the modified Bridgman method, were measured at room temperature. The standard and modified Judd–Ofelt theories, extended to anisotropic crystal, have been applied to analyze the spectra. The spectroscopic parameters, including the Judd–Ofelt intensity parameters _t(t=2,4,6), spontaneous emission probabilities, fluorescence branching ratios, radiative lifetimes, stimulated emission cross sections, and fluorescence quantum efficiencies, were estimated. The good spectroscopic properties show the possible application of the Pr³⁺-doped PbWO₄ crystal as solid-state and self-stimulated Raman laser materials. PACS 78.20.-e; 42.70.Hj     

Spectroscopic characteristics of Pr<Superscript>3+</Superscript> in biaxial La<Subscript>2</Subscript>(WO<Subscript>4</Subscript>)<Subscript>3</Subscript> crystal

A Pr³⁺-doped La₂(WO₄)₃ crystal grown by the Czochralski method has been investigated as a promising laser material. The principal axes of the optical indicatrix and Pr³⁺ concentration of the crystal were determined. The polarized absorption, fluorescence spectra and fluorescence decay curves of the main emission multiplets of the crystal were measured at room temperature. The spectroscopic parameters were obtained by the modified Judd–Ofelt theory combined with the normalized method. The peak stimulated emission cross-sections of the major emission lines were estimated. The good spectroscopic properties imply that the Pr³⁺:La₂(WO₄)₃ crystal is a potential laser gain medium for solid-state laser and self-stimulated Raman laser applications. PACS 78.20.-e; 42.70.Hj     

Impurity effect on the Raman spectra of Sr0.6Ba0.4Nb2O6

Impurity effect on the rare earth ion doped Sr_0.6Ba_0.4Nb₂O₆(SBN40) was studied at room temperature. Doping the rare earth ions of Pr³⁺ or Nd³⁺ changed the Raman profile: spectral broadening, central frequency shifts and relative intensity decreasing. Two reasons are considered according to the ferroelectric and optical properties of the rare earth ion doped SBN40: impurity-induced crystal disorder and the crystal structure change. SBN40 is the general disorder crystal and the disorder which is enhanced by doping the rare earth ion is especially strong along the x?y plane of the material compared with that along the polar C-axis.     

Spectral properties of Pr3+ ions in Bi2(MoO4)3 crystal

A Bi₂(MoO₄)₃ single crystal doped with Pr³⁺ ions has been grown by the Czochralski technique. The polarized absorption and fluorescence spectra as well as the fluorescence decay curve of Pr³⁺ ions in the crystal were measured at room temperature. The spectroscopic parameters, including the Judd–Ofelt intensity parameters Ω_t (t=2, 4, and 6), spontaneous emission probabilities, fluorescence branching ratios, radiative lifetimes, stimulated emission cross sections, and fluorescence quantum efficiencies, were calculated. The spectral properties related to laser performance of this crystal were analyzed. The ¹ D ₂ multiplet of the crystal may be a good upper level for a solid-state laser.     

A study of the fluorescence lifetime of Pr3+ in SBN40

The fluorescence lifetime τ₁ of Pr³⁺ doped in the ferroelectric solid solution SNB40 (Ba_0.4Sr_0.6Nb₂O₆) was measured ar various temperatures. The fluorescence lifetime decreases gradually with increasing temperature. Furthermore, an anomalous increase of τ₁ was observed at a specific temperature. The fluorescence linewidth and the peak wavelength of fluorescence also showed an anomalous change at this temperature. It is likely that this phenomenon is due to the phase transition of the host crystal SBN40.     

Inverse Raman spectra of SBN40+Pr3+

Inverse Raman spectra of rare-earth ion doped SBN40 [Ba_0.4Sr_0.6Nb₂O₆:Pr³⁺(1.0 weight%)] are obtained over a range 0 to 950 cm^?1 using an Ar ion laser and a pulse-dye laser with 0.2 micros pulsewidth. The spectra are in agreement with the results obtained by the normal Raman scattering. It is found that a single-shot IRS is possible to obtain the Raman spectrum within laser exposuring time, if it is a sharp one.     

Absorption and fluorescence intensity analysis of Pr3+ in LiPrP4O12 crystal

Absorption and fluorescence spectra of LiPrP₄O₁₂ crystal were measured with high accuracy. Using the Judd-Ofelt theory the Ω_λ parameters and probabilities of the radiative transitions for the ³P₀, ¹D₂, excited states were calculated. From the presented analysis of the fluorescence spectra of Pr³⁺ ions, we conclude that there are two unequivalent positions in LiPrP₄O₁₂ crystals.     

Spectral-kinetic characteristics of Pr luminescence in LiLuF4 host upon excitation in the UV-VUV range

Spectral-kinetic study of Pr³⁺ luminescence has been performed for LiLuF₄:Pr(0.1 mol%) single crystal upon the excitation within 5-12 eV range at T=8 K. The fine-structure of Pr³⁺ 4f ²→4f 5d excitation spectra is shown for LiLuF₄:Pr(0.1 mol%) to be affected by the efficient absorption transitions of Pr³⁺ ions into 4f 5d involving 4f ¹ core in the ground state. Favourable conditions have been revealed in LiLuF₄:Pr(0.1 mol%) for the transformation of UV-VUV excitation quanta into the visible range. Lightly doped LiLuF₄:Pr crystals are considered as the promising luminescent materials possessing the efficient Pr³⁺³P₀ visible emission upon UV-VUV excitation. The mechanism of energy transfer between Lu³⁺ host ion and Pr³⁺ impurity is discussed.