Tm3+掺杂硅酸镓镧(La3Ga5SiO14)晶体的结构与光学性能研究

利用X射线粉末衍射确定了Tm³⁺掺杂硅酸镓镧(La₃Ga₅SiO₁₄,LGS)晶体的晶体结构;运用DICVOL91程序计算了该晶体不同部位的晶胞参数;测定了Tm：LGS晶体的室温吸收谱和470nm光激发下的发射光谱;根据Judd-Ofelt理论拟合了Tm³⁺的三个晶场调节参数Ω_t(t=2,4,6),分别为2.694×10^-20cm²,1.842×10^-20cm²,0.030×10^-20cm²;计算了各个能级跃迁的谱线强度、振子强度、吸收截面等,进而计算了³H₄和³F₄态的自发跃迁概率、辐射寿命、荧光分支比和积分发射截面,并对结果进行了分析. 关键词： Tm：LGS晶体 吸收谱 Judd-Ofelt理论 光谱参数     

用Judd-Ofelt理论计算TmP5O14晶体中Tm3+的光谱参数

根据Judd-Ofelt理论,测得了Tm3+ 在TmP5O14晶体中的强度参数分别为Q2=:1.50×10-20cm2,Q4=1.51×10-20cm2,Q6=0.916×10-20cm2,计算的振子强度Pcal.与实验值Pexp.符合较好,平均根方误差为2.60×10-7。求得Qλ后,计算了J多重激发态之间的振子强度,自发辐射跃迁速率,辐射寿命和荧光分支出,与YAlO3:Tm3+,YAG:Tm3+、Y2O3:Tm3+等晶体和掺Tm3+玻璃的光谱参数进行了比较,并就3H4→3H6,3F4→3H5,1D2→3H4和1G4→3H4的跃迁进行了对比和讨论。观察到Tm3+在不同介质中的Pexp.与强度参数的总和∑τλ=τ2+τ4+τ6存在Pexp=α∑τλ+b的关系。     

钨酸钇钠晶体中Tm3+的光谱特性

测量了Tm3 :NaY(WO4 ) 2 晶体的吸收光谱、发射光谱和激发光谱 ,利用J_O理论计算了钨酸钇钠晶体的强度参数 :Ω2 =7 2 130 4× 10 - 2 0 cm2 ,Ω4 =0 5 0 4 76 6× 10 - 2 0 cm2 ,Ω6 =0 977784× 10 - 2 0 cm2 ,以及Tm3 的光学参数包括各能级的荧光寿命和荧光分支比、积分发射截面等 ,在计算了Tm3 的自发辐射概率时 ,同时考虑了电偶极跃迁和磁偶极跃迁 .研究了其发光特性和跃迁通道 ,发现存在1 D2 3H6 →1 G4 3F4 的交叉弛豫     

Er:YCa4O(BO3)3光谱参数的计算及分析

测定了Er:YCa4O(BO3 ) 3 晶体室温下的吸收谱。根据Judd Ofelt理论拟合了Er3 离子的晶体场调节参数Ωt=(2 ,4 ,6 ) 分别为 19 2 0 4 9× 10 -2 2 ,5 992 0× 10 -2 2 和 4 3334× 10 -2 2 cm2 ,计算了各能级跃迁的谱线强度、自发辐射跃迁几率、辐射寿命、荧光分支比和积分发射横截面 ,并对结果作了分析。最后讨论了Yb3 的敏化作用。     

Tm3+/Yb3+共掺铋碲酸盐玻璃中的高效蓝色上转换荧光

制备了高折射率Tm3+/Yb3+共掺杂铋碲酸盐玻璃,利用棱镜耦合法测量出玻璃在632.8和1550 nm波长处的折射率分别为2.0365和1.9795. 对玻璃的吸收、荧光和红外透过光谱展开了测试与分析,根据Judd-Ofelt理论对吸收光谱进行拟合,求得Tm3+的振子强度参数Ωt(t=2,4,6)分别为3.90×10-20, 2.03×10-20和9.03×10-21 cm2,并进一步计算了Tm3+在玻璃中各能级跃迁的振子强度、自发辐射跃迁概率、辐射寿命和荧光分支比等光谱参数. 在980 nm激光激发下测得强的蓝色三光子上转换和近红外双光子上转换荧光. 宽的红外透过窗口、高的折射率和强的蓝色上转换荧光表明,Tm3+/Yb3+共掺铋碲酸盐玻璃有希望成为高效的上转换发光和激光材料.     

Er~(3+):Ba_(0.65)Sr_(0.35)TiO_3纳米粉体光谱性质

用溶胶-凝胶法制备了Er3+:Ba0.65Sr0.35TiO3(BST)纳米粉体,测试了纳米粉体在室温下的吸收光谱与光致发光谱。利用Judd-Ofelt理论拟合得到晶体场强度参数Ω2,Ω4和Ω6分别为0.993×10-20,1.665×10-20和0.540×10-20cm2,系统计算了Er3+能级跃迁的谱线强度、自发辐射跃迁概率、荧光分支比等光谱参数。发光谱表明,样品出现了中心波长位于522,545,654和851nm的发光带,分别对应Er3+的2H11/2→4I15/2,4S3/2→4I15/2,4F9/2→4I15/2和4S3/2→4I13/2的跃迁。讨论了样品的发光特性。结果表明Er3+:BST纳米材料在新型光电子器件中有广泛的应用前景。     

Tm:YVO4晶体的光谱参数计算

由测量的Tm :YVO4晶体的吸收光谱 ,考虑到单轴晶体在各个方向上的吸收不同和折射率随波长的变化 ,根据Judd Ofelt理论计算了Tm3 +在YVO4中的强度参数、各个能级的振子强度、自发辐射几率、荧光分支比、积分发射截面等参数。强度参数为Ω2 =1 9416× 10 - 2 0 (cm2 ) ,Ω4=0 15 6 8× 10 - 2 0 (cm2 ) ,Ω6=0 396 3× 10 - 2 0 (cm2 )。计算结果表明 ,1 D2 → 3 F4的跃迁几率远大于1 D2 向其他各个能级的跃迁几率     

掺Tm钒酸钇的光学性能

钒酸钇(YVO4)晶体有高的激光损伤阈值和高的激光输出斜率效率,也有很好的机械性能和化学稳定性.从测量TmYVO4晶体的吸收谱入手,考虑该晶体的各向异性效应,拟合出Tm3+的光学强度参量,进一步得到了振子强度f,辐射跃迁速率A和积分发射截面Σ等光学参量.在350-2500nm范围内,YVO4晶体基质的吸收很小,而Tm3+在YVO4晶体中发光能力很强;特有的是蓝光1D2→3F4(约为454nm)跃迁有极大的振子强度(38×10-6)和积分发射截面(33×10-18cm),有利于实现短波长的激光输出.     

HO3+/Tm3+共掺α-NaYF4单晶体的光谱特性

采用坩埚下降法生长出Ho3+离子掺杂浓度～1.90 mol％、Tm3+不同掺杂离子浓度(0.99 mol％,1.58 mol％,2.37 mol％,3.16 mol％,3.99 mol％,7.19 mol％)的双掺杂立方晶相NaYF4单晶体.根据测定的吸收光谱以及800 nmLD波长激发下的发射光谱、发射截面和衰减曲线,研究从Tm3+离子到Ho3+离子的能量传递机制、Tm3+离子的浓度猝灭效应和Ho3+离子在2.04 μm波段的优化发光效应.当Ho3+离子浓度保持为～1.90 mol％不变,Tm3+离子浓度从0.99 mol％增加到1.59 mol％时,2.04 μm波段的发射强度逐步增强;当浓度从1.59mol％增加到7.19mol％时,发射强度逐步减弱.Ho3+ (1.90 mol％)/Tm3+ (1.59 mol％)共掺的单晶体的发射截面最大,达到2.17×10-20 cm2,其荧光寿命最长,为21.72 ms;同时,根据Ho3+离子的吸收截面和Tm3+离子的发射截面,计算得到该样品从Tm3+:3F4→Ho3+:5I7稀土离子能量传递系数和Ho3+:5I7→Tm3+:3F4反传递系数分别为CTm-Ho=24.14×10-40 cm6/s,CHo-Tm=2.05×10-40 cm6/s.     

Ho3+:LiYF4晶体的中红外发光特性

用坩埚下降法制备了Ho3+离子掺杂的LiYF4单晶。测定了Ho3+:LiYF4晶体的偏振吸收光谱。应用Judd-Ofelt理论分别计算了Ho3+:LiYF4晶体中Ho3+离子的有效强度参数Ω2,4,6、能级跃迁振子强度fexp和fcal、自发辐射跃迁几率A、荧光分支比β、辐射寿命τrad等光谱参数。测定了样品在640 nm光激发下的红外发射光谱,观测到由Ho3+离子的5I6→5I7跃迁所致的2.8～3μm中红外发光,以及在1.2μm(5I6→5I8)和2.0μm(5I7→5I8)处较强的荧光。Ho3+:LiYF4单晶样品的吸收峰线宽较宽,计算得到1.2μm和2.0μm的峰值发射截面分别达到0.20×10-20cm2和0.51×10-20cm2,同时测定了1 191 nm(5I6→5I8)和2 059 nm(5I7→5I8)发射的荧光寿命。研究结果表明:Ho3+:LiYF4晶体在2.0～3μm波段的中红外激光器中有较大的应用前景。     

Fine structure and isotope shift of the 3s4d 3 D-3s3p 3 P, 3s5d 3 D-3s3p 3 P and 3p 2 3 P-3s3p 3 P Transitions of MgI

Summary We report the measurements of the³ D(3s4d)-³ P(3s3p)³ D(3s5d)-³ P(3s3p), and³ P(3p ²)-³ P(3s3p) transition frequency of MgI, the fine-structure separation and isotope shift between²⁴Mg and²⁶Mg. The measurements have been performed in a metastable atomic beam; a good agreement is found for data already existing in the literature. The accuracy of the measurements reported in this paper is mainly limited by the Doppler broadening of theI ₂ transitions used as a reference and by the precision in the knowledge of the related wavelengths.     

The gas phase infrared band contours of s-triazine and s-triazine-d3: The fundamentals of C3N3H3 and C3N3D3 and some overtone and combination bands of C3N3H3

The systematic application of band contour techniques to account for most of the observed features of the ir spectra of s-triazine and s-triazine-d₃ have been made as well as a critique as to the limitations of such methods. The experimental and computer methods used to study the gas phase infrared band contours of s-triazine and s-triazine-d₃ are out-lined. Contours of the five E′ fundamentals of s-triazine have been recorded under moderate resolution and analyzed to give the Coriolis constants $\text{ζ}{}_{\mathrm{i}}{}^{\mathrm{z}}$, i = 6–10. The effects of l-resonance are very apparent for ν₈ and ν₉, in the form of holes in the Q branches of these bands. Under the highest resolution available, ν₆ and ν₁₀ also show l-resonance effects. Values of the l-doubling constants $\text{q}{}_{\mathrm{i}}{}^{\mathrm{(+)}}$ were obtained for these four fundamentals. One of the parallel A₂″ fundamentals of C₃H₃N₃ (ν₁₂) has also been studied. It lies close to ν₁₀(E′) and an A × E type of second-order Coriolis resonance may be the cause of the intensity enhancement observed in the inner wings of the ν₁₂ and ν₁₀ bands. Hot bands of the type (ν_i + nν₁₄ ? nν₁₄) have been observed in the contours of ν₈, ν₁₀, and ν₁₂. This is felt to be responsible for the large difference between our observed zeta sum (?1.30) and the theoretical sum (?1.00).The gas phase infrared band contours of the five E′ and 2A₂″ fundamentals of C₃N₃D₃ have also been recorded under moderate resolution. From P-R separations and by computer simulation of the contours, values of the Coriolis constants $\text{ζ}{}_{\mathrm{i}}{}^{\mathrm{z}}$ have been obtained for the E′ modes. The effects of l-resonance have been observed for ν₈(E′) and ν₁₀(E′) and values of the l-doubling constants $\text{q}{}_{\mathrm{i}}{}^{\mathrm{(+)}}$ have been estimated. An extensive series of hot bands of the type (ν₁₂ + nν₁₄ ? nν₁₄) has been observed in the contour of the ν₁₂ (A₂″) fundamental. The mass effect on the Coriolis constants has been discussed.Infrared band contours of the overtone 2ν₇ and seven degenerate E′ combination bands of C₃N₃H₃ have been recorded under moderate resolution. Analysis of these contours using the P-R separation method and computer simulation of the contours has given values of $\text{ζ}{}_{\mathrm{<mtext>eff</mtext>}}{}^{\mathrm{z}}$ for these bands. Fermi resonance between 2ν₇ and ν₆ has been analyzed. The importance of considering both the observed contour as well as the observed frequency when assigning higher tone bands is illustrated.     

Dielectric investigations of solid solutions SrTiO3-KTaO3 and SrTiO3-KNbO3

The temperature dependences of the dielectric constant and dielectric hysteresis loops in ceramic samples of (1 ? x)SrTiO_3?x KNbO₃ and (1 ? x)SrTiO_3?x KTaO₃ (0 ≤ x ≤ 0.3) solid solutions prepared using different heat treatments have been investigated. Phase diagrams of the studied solid solutions have been constructed in the T-x coordinates. It has been shown that, after quenching of samples (spontaneous cooling at room temperature after long-term heating at the sintering temperature of the ceramic samples), the temperature of the induced phase transition increases because of the weakening of random electric fields associated with nonisovalent impurities due to their “frozen” nonequilibrium redistribution. For small concentrations x, strong dielectric relaxation is observed in the temperature range of 150–250 K. A model of relaxing centers, which is based on the local charge compensation of heterovalent impurities, has been proposed.     

Infrared spectra of matrix isolated BH3NH3, BD3ND3, and BH3ND3

The infrared spectra of ammonia-borane, BH₃NH₃, and two of its deuterated isotropic species, BD₃ND₃ and BH₃ND₃, isolated in argon matrix at liquid hydrogen temperature have been measured. Well resolved bands for these three isotopic species have been observed for all the fundamentals. A complete frequency assignment based on C₃v molecular symmetry has been made. A set of force constants have been calculated from the data for the two isotopes BH₃NH₃ and BD₃ND₃ using a valence force field. The agreement between experiment and frequencies calculated from these force constants for the mixed isotopic species, BH₃ND₃, substantiates the present assignment.     

LaGaO3:RE3+(RE3+=Eu3+,Ho3+)的光谱

本文用固态反应合成了钙钛矿型的LaGaO3和LaGaO3:RE3+(RE3+=Eu3+,Ho3+)荧光体,并观察了物相随不同的激活离子浓度的变化。测量了化合物在室温下的反射光谱,激发光谱和荧光光谱。研究了Eu3+的D0→7F2和Ho3+的5S2→5I8的荧光强度与激活离子浓度的关系,发现了浓度猝灭,并得到了最大荧光强度的浓度值。     

Terahertz Vibrational Modes in CH3NH3PbI3 and CsPbI3 Perovskite Films

JETP Letters - Films of CH3NH3PbI3 organometallic perovskite, which is currently considered as a promising basic material for new-generation solar cells, as well as films containing CsPbI3...     

Ba3La(BO3)3基质中Tb3+的光致发光

以高温固相法合成了Ba3La(BO3)3∶Tb3 发光材料。在254nm紫外光激发下,研究了Ba3La(BO3)3∶Tb3 的激发光谱、发射光谱、发光强度与Tb3 浓度的关系。确定了Ba3La(BO3)3基质中Tb3 的自身浓度猝灭机理;探讨了助熔剂LiCO、敏化剂Ce3 、Bi3 的加入对荧光粉的发光强度的影响。     

Modulated magnetic structures of ErPb3, HoPb3, ErTl3 and HoTl3

Neutron diffraction experiments have been carried out on the magnetically ordered phases of ErPb₃, HoPb₃, ErTl₃ and HoTl₃. The magnetic moments were found to be sinusoidally modulated with a propagation vector of (0, 0.2, 0.5) for the Pb-compounds and (0.38, 0.38, 0.16) for the Tl-compounds.Work supported by the Bundesministerium für Forschung und Technologie     

（LaO）3BO3中Eu^3＋和Sm^3＋的光致发光

研究了紫外光激发下，（ＬａＯ）３ＢＯ３基质中Ｅｕ＾３＋和Ｓｍ＾３＋的光谱性质，Ｅｕ＾３＋和Ｓｍ＾３＋的电荷迁移激发带及发光强度随组成和结构变化的规律性，并探讨了Ｅｕ＾３＋和Ｓｍ＾３＋自身浓度猝灭的机理。