LiNbO3:MgO晶体的喇曼光谱研究

首次获得了LiNbO₃:MgO晶体的喇曼光谱。与纯LiNbO₃晶体的喇曼光谱相比较,A₁(TO)模和E(TO)模的谱线数目、频率和相对强度均基本不变,线宽略有增加。这说明,LiNbO₃晶体较强的A₁(TO)和E(TO)振动模的喇曼光谱主要是由氧八面体(NbO₆)特征基团所贡献的。 关键词：     

BaTiO3和Ce:BaTiO3晶体极性声子和电磁激元的喇曼散射研究

从声子-电磁激元频率色散关系的普遍公式出发,推导出了单轴晶体的Merten方程和电磁激元的频率色散关系。测量了BaTiO₃和Ce:BaTiO₃晶体的简正模和斜声子的喇曼散射谱,并根据Merten方程,拟合出了斜声子的方向色散曲线;记录了A₁类电磁激元在不同波矢值下的喇曼谱,观察到其频率色散现象.根据以上结果,对A₁(TO)模喇曼谱中两个宽的非对称峰的归属和BaTiO₃晶体的结构相变机制进行了讨论;计算出了这两种晶体的受夹介电常数;分析了掺Ce对BaTiO₃晶体结构的影响。 关键词：     

钛-硅系快速热退火固相反应机制的研究

钛膜在10^-7Torr真空中用电子束蒸发沉积在硅单晶片上,以快速热退火方式进行团相反应。转靶X射线衍射分析发现,540—600℃退火后,有两个亚稳相Ti₅Si₄的衍射峰。延长退火时间,第一成核相Ti₅Si₄可持续存在到钛被消耗完,随即转变成稳定相TiSi₂。退火温度高于640℃,形成稳定相TiSi₂。薄层电阻和喇曼散射的测量研究结果表明,与X射线衍射有很好的对应。207和244cm^-1波数处的两个喇曼峰为TiSi₂的特征喇曼峰,而270,297和341cm^-1的三个喇曼峰似乎是由Ti₅Si₄引起。 关键词：     

c向静电场作用下α-LiIO3单晶的喇曼谱“串线”和谱线强度改变的机理

在c向静电场作用下,α-LiIO₃单晶的喇曼谱发生“串线”,并且谱线强度改变。本文分析了这一现象的起因:由于离子输运引起的空间电荷涨落使α-LiIO₃单晶的极化率张量和喇曼张量主轴方向发生涨落。前者产生o←→e光散射,散射光再发生一次喇曼散射,造成喇曼谱“串线”和谱线强度的改变;后者直接造成喇曼诺“串线”和谱线强度的变化。前者的贡献远大于后者。 关键词：     

KTiOPO4晶体纵横模劈裂的喇曼谱

在室温下测量了ＫＴｉＯＰＯ₄单晶的偏振喇曼散射谱，应用９０°散射及背散射得到了各模的峰位值，其中Ｂ₁（ＬＯ）模、Ｂ₂（ＬＯ）模的喇曼谱测量尚未见报道过。根据ＬＯ－ＴＯ劈裂的实验结果，计算出该晶体极化模的有效电荷、振子强度及沿对称轴方向的静态介电常数。 关键词：     

纳米尺寸下Pb1-xBaxTiO3的喇曼振动光谱及软模行为的研究

测量了Pb_1-xBa_xTiO₃(x=0,0.2,0.3)的喇曼光谱。实验结果表明该体系存在着明显的晶粒小尺寸效应。 关键词：     

LiYF4:Nd3+的电子喇曼散射与双光子荧光

首次观察到下列LiYF₄:Nd³⁺的光谱:用波长λ为4880?的Ar⁺激光激发的⁴I_11/2能级所属斯塔克子能级Y₁—Y₆的电子和电-声子喇曼散射谱;用波长λ为6943?的红宝石激光激发的双光子荧光和电-声子荧光谱。 关键词：     

高压H2受激喇曼散射的阈值与能量转换效

我们着重研究了高压H₂气Q(1)振动跃迁(4155cm^-1)受激喇曼散射(SRS)中,参与非线性相互作用的几个参数(介质分子密度、跃迁线宽、泵浦光子密度以及非线性作用长度)对受激阈值与能量转换效率的影响。给出了自零到24atmH₂气压范围内阈值随H₂气压变化的实验结果,它与根据Dicke-Doppler展宽和碰撞展宽的联合效应的分析是一致的。讨论了由于受激喇曼过程(SRP)和四波混频参量过程(FWPP)共同影响下能量转换效率、压力-色散效应对高阶反斯托克斯的能量输出的重要影响。 关键词：     

LaxBi2-xTi4O11的合成及相变研究

合成了Ｌａ_xＢｉ_2-xＴｉ₄Ｏ₁₁系列样品，并完成了它们的喇曼光谱和ｘ射线衍射测量；结果表明，该体系在Ｘ＝１．２经历了一次相变，且相变与最低频声子模随Ｘ的变化有关。Ｌａ_0.2Ｂｉ_1.8·Ｔｉ₄Ｏ₁₁的相变温度为２００℃。初步获得Ｌａ₂Ｔｉ₄Ｏ₁₁的结构为正交结构。 关键词：     

高压H2的SRS中的参量与非参量过程

本文报道了在数十气压H₂中输出三级Stokes和六级anti-Stokes受激喇曼散射。着重研究了SRS能量转移中的受激喇曼过程(SRP)和四波参量过程(FWPP)。对前人报道得很少的高压H₂中的离轴Stokes圆环与轴上anti-Stokes圆斑进行了较系统的实验研究,并用非线性光学参量与非参量过程的有关理论对实验结果进行了讨论。 关键词：     

RAMAN STUDY ON (Pb) CENTERS IN SINGLE CRYSTALS OF ALKALI HALIDES DOPED WITH LEAD

Low frequency modes were observed in a series of alkali halides doped with lead after X-irradiation at 77K. The peak positions of the Raman signals are at 34cm^-1 for NaCl:Pb²⁺, 30cm^-1 for KCl:Pb²⁺,28cm^-1 for RbCl:Pb²⁺ and 22cm^-1 for KBr:Pb²⁺. They are assigned to the inelastic light scattering caused by the local vibration of X^-_i (Pb⁺) center, which consists of an interstitial halogen ion stabilized by a substitutional ion Pb⁺ . Polarized Raman measurements and Behavior Typer(BT) analysis show that the symmetry of the X^-_i (Pb⁺) center belongs to the point group C_3v A structure model of the X^-_i (Pb⁺) center is proposed based on the Raman data and the result of BT analysis.     

Emission and decay time studies on Pb2+ centers in KBr,RbBr, and RbCl

The emission spectra and the luminescence decay times of KBr, RbBr, and RbCl crystals doped with Pb²⁺ and excited in the A-absorption band have been studied in the temperature range 5–300 K. The emission-lineshape spectra have been analysed in terms of skew-Gaussian bands. New bands have been observed in RbCl and RbBr at very low temperatures. While the luminescence decay of KBr:Pb²⁺ and RbBr:Pb²⁺ show only a single component with a decay time τ ～ 20 ns, RbCl:Pb²⁺ shows a short and a long component. The reason for the missing long component in KBr:Pb²⁺ and RbBr:Pb²⁺ is tentatively attributed to an anomaly in the structure of the adiabatic potential energy surface (APES) of the excited states.     

Radiative energy transfer from Pb2+ to Eu2+ ions in NaCl,Kcl, and KBr single crystals

In the present work, the emission and excitation spectra of NaCl, KCl, and KBr doubly doped with europium and lead ions were investigated. In all cases, excitation with light lying in the A-band of the Pb²⁺ ions produces in addition to the ³P₁ → ³S_o Pb²⁺ emission, the 4f⁶ 5d (^t2g) → 4f⁷ europium emission. This fact indicates that energy transfer occurs from Pb²⁺ to Eu²⁺ ions. From the data obtained, it was determined that the energy transfer process is of a radiative nature and that it is more efficient in KCl than in either of NaCl or KBr. A possible explanation for this fact is given.     

A novel blue-emitting phosphor: BaAl2B2O7: Pb

Pb²⁺ doped BaAl₂B₂O₇ materials were prepared by a solution combustion synthesis. The phase of the synthesized materials was determined using the powder X-ray diffraction. The photoluminescent properties of Pb²⁺ doped BaAl₂B₂O₇ materials were investigated using spectrofluorometer at room temperature. The emission and excitation bands of BaAl₂B₂O₇: Pb²⁺ were observed at 423 and 266 nm, respectively. The dependence of the emission intensity on the Pb²⁺ concentration for BaAl₂B₂O₇: Pb²⁺ was investigated. The Stokes shifts of BaAl₂B₂O₇: Pb²⁺ was calculated to be 13 953 cm⁻¹.     

Barium borate glass and transparent glass ceramics doped with Pb4Lu2YbF17

Barium borate glasses doped with complex Pb₄Lu₂YbF₁₇ fluoride have been synthesized and investigated. Heat treatment produced glass ceramics containing the crystalline BaF₂:Yb³⁺ phase. The changes in the structural and optical properties of the glass ceramics were revealed by X-ray diffraction, Raman spectroscopy, and luminescence spectroscopy of Yb³⁺ ions in polycrystalline Pb₄Lu₂YbF₁₇, initial glass, and glass ceramics.     

Rietveld refinements and vibrational spectroscopic studies of Na1−xKxPb4(PO4)3 lacunar apatites (0≤x≤1)

Synthesis of apatites, Na_1−xK_xPb₄(PO₄)₃ 0≤x≤1, with anion vacancy was carried out using solid state reactions. The solid solution of apatite-type structure crystallizes in the hexagonal system, space group P6₃/m (No 176). Rietveld refinements showed that 75% of Pb²⁺ cations are located in the (6h) sites; the ninefold coordination sites (4f) are equally occupied by the other 25% lead cations and the K⁺ and Na⁺ monovalent ions.The structure can be described as built up from [PO₄]³⁻ tetrahedra and Pb²⁺ of sixfold coordination cavities (6h positions), which delimit void hexagonal tunnels running along [0 0 1]. These tunnels are connected by cations of mixed sites (4f) half occupied by Pb²⁺ and half by Na⁺/K⁺ mixed cations. The assignment of the observed frequencies in the Raman and infrared spectra is discussed on the basis of a unit cell group analysis and by comparison with other apatites. The Raman modes of all the compositions show some linear shifts of the frequencies as a function of the composition toward lower values due the substitutions of Na⁺ by K⁺ with a larger radius.     

Electronic and vibrational spectra of MnO2−4 in KBr crystals

Two new features have been observed in the electronic spectrum of KBr crystals doped heavily with MnO^2?₄ ions. The band at 870 nm is assigned to the crystal field transition e → t₂. The band at 600 nm shows a series of vibrational sub-bands at an interval of 740cm^?1 and is ascribed to the coupling between electronic transition and totally symmetric mode of the ion.A line at 830cm^?1, ascribed to totally symmetric mode v₁(A₁), has been observed for the first time in the Raman spectrum. I.R. spectrum of KBr: MnO^2?₄ shows four lines—one due to MnO^2?₄ in Td symmetry and the other three to the split components of v₃(T₂) for MnO^2?₄ in Cs symmetry. I.R. spectrum of KBr: MnO^2?₄: Ca²⁺ shows another s of four lines—one due to MnO^2?₄ in Td symmetry and the other three to the v₃(T₂) mode of the ion in C_2v symmetry. The v₁(A₁) line could not be observed in the i.r. spectra.     

Polarized Raman and IR spectra of non‐centrosymmetric PbB4O7 single crystal

Polarized Raman and IR spectra of a PbB₄O₇ single crystal were measured. The obtained spectra are discussed within the factor group approach for the orthorhombic P2₁nm(C_2v⁷) space group with Z = 2 assuming that the crystal structure is built up of the (B₄O₇)_∞²⁻ framework and Pb²⁺ ions. It has been shown that vibrations of borate and Pb²⁺ units are observed above 240 and below 160 cm⁻¹, respectively. The results obtained for the spontaneous Raman scattering have also been used in the discussion of the stimulated Raman spectra of the material studied—a new Raman‐laser crystal. The obtained results revealed that mainly translational motions of Pb²⁺ ions participate efficiently in the SRS effect. Copyright © 2008 John Wiley & Sons, Ltd.     

Absorption- and uniaxial stress experiments in the a band of Pb2+ centres in KBr,RbBr, KI and RbI

The absorption lineshape and the stress induced dichroism of the A band of Pb²⁺ centres in KBr, RbBr, KI and RbI have been measured as a function of temperature from 4 K to room temperature. The moments of the absorption bands and of the dichroic spectra have been determined, and the effective coupling constants of the linear electron-lattice interactions of the ¦A〉 state as well as the frequencies of the interaction modes have been evaluated. Above 200 K the temperature dependence of the moments gives strong evidence that nonlinear electron-lattice interactions are important, particularly in the case of KBr:Pb²⁺.     

Optical absorption of s2-configuration ions in alkali halide crystals—III: The A band in Sn2+-doped crystals

The line shape of the A band in KCl:Sn²⁺, KBr:Sn²⁺, KI:Sn²⁺, RbCl:Sn²⁺ and RbBr:Sn²⁺ has been measured as a function of temperature between about 15 K and room temperature. As the spectra for all these systems are similar detailed results are presented only for RbCl: Sn²⁺, RbBr:Sn²⁺ and KBr: Sn²⁺. The experimental data resemble those of a previous study on KBr:In⁺ and KG:In⁺ in that the A band consists of two broad, overlapping components designated A₁ (the low energy component) and A₂. The separation between A₁ and A₂ is more marked at low temperature for Sn²⁺ than for In⁺, and no inversion of the ratio of the peak heights of A₁ and A₂ occurs as the temperature is varied, as was so for In⁺. Detailed calculations of the line shape are presented for KBr:Sn²⁺. These calculations show that one cannot account for the line shape purely in terms of the dynamical Jahn-Teller effect and that there is in addition a static splitting of the A state caused by a lowering in the symmetry of the crystal field.