NH4NO3掺杂Na^＋,K^＋,Ag^＋,Pb^2＋晶体相变拉曼峰强行为研究：掺杂效 …

从掺杂晶体（Ｎａ＾＋，Ｋ＾＋Ａｇ＾＋，Ｐｂ＾２＋）ｘ（ＮＨ４）１－ｘＮＯ３相变时，拉曼峰强与温度的变化关系着手，深入人了掺杂离子效应，揭示了其中的标度性质，本文分不下列算：（１）前言，（２）实验；（３）ｌｎＩｒ与Ｉｎ│Ｔ－Ｔｃ│之线性关系，（４）不同振动模对不同掺杂程度的反应；（５）ｖ１振动模对不同离子掺杂的刻画；（６）反转行为，（７）ｄｃ与Ｍ＾１／２的线性关系。（８）掺杂效应的标度性，（９）结语     

关于从拉曼峰强研究分子晶体及其掺杂体系相变工作的几点总结

本文总结了近年我们有关从拉曼峰强来研究分子晶体及其掺杂体系相变的工作。文中重点强调工作出发点的思路和观点以及未来的展望。其中着重介绍拉曼峰强的指数函数行为，相变的分形观点以及掺杂的表征等。     

关于从拉曼峰强研究分子晶体及其掺杂体系相交工作的几点总结

本文总结了近年我们有关从拉曼峰强来研究分子晶体及其掺杂体系相变的工作［１－４］。文中重点强调工作出发点的思路和观点以及未来的展望．其中着重介绍拉曼峰强的指数函数行为，相交的分形观点以及掺杂的表征等。     

自受激拉曼晶体Nd3+:SrMoO4的光谱性质研究

通过拉曼散射光谱,吸收光谱,荧光发射寿命和808 nm LD激发下的红外荧光光谱的实验测量,系统研究了Nd3+:SrMoO4晶体的自受激拉曼光谱性质.分析指认了拉曼散射光谱中各拉曼峰所对应的晶格振动模式,得出了其SRS活性最强的声子频率约为898 cm-1,对应于(MoO24-)离子团的完全对称光学伸缩振动Ag模;通过J-O理论对晶体的吸收谱进行了全面的光谱参数计算,得出4F3/2→I11/2跃迁的积分发射截面达O.57×10-18cm2,自发辐射概率为141.06s-1;同时,实验测得该跃迁的荧光发射寿命约为O.2 ms.最后,结合808 nm LD激发下的红外波段荧光光谱,论证了SrMoO4晶体中Nd3+离子1068 nm发射通过拉曼频移获得1180 nm一级斯托克斯激光发射的可能性,为Nd3+:SrMoO4晶体的自受激拉曼激光器研究提供了理论依据.     

沉淀法制备Li~+、Na~+掺杂Gd_2O_3:Eu~(3+)荧光粉及发光特性研究

用沉淀法制备Li~+、Na~+和Eu~(3+)共掺Gd_2O_3荧光粉,并与微波-固相法制备的样品进行了比较。通过测量该粉体的XRD、激发光谱和发射光谱,比较了样品的微观结构和讨论了不同合成条件对Gd_2O_3:Eu~(3+)荧光粉发光特性的影响。结果显示在相同的条件下,对于未掺入Li~+的Gd_2O_3:Eu~(3+)样品比较,沉淀法制备样品的发光强度是微波-固相法制备样品的1.68倍;掺入Li~+的Gd_2O_3:Eu~(3+)样品比较,沉淀法制备样品的发光强度是微波—固相法制备样品的1.82倍。当使用草酸作为沉淀剂,掺杂浓度为Li~+(4.5 mol%)、Na~+(4.5mol%)、Eu~(3+)(4.5mol%),在800℃煅烧2h后获得样品的发光强度,是Gd_2O_3:Eu~(3+)荧光粉的5.91倍。     

Li+共掺杂GdTaO4:Eu3+发光增强效应的研究

测量了不同浓度Li+共掺杂下GdTaO4:Eu3+荧光粉材料的X射线衍射谱(XRD)、发射光谱以及红外透射谱,并应用Judd-Ofelt理论,由发射光谱得到Eu3+的光谱跃迁强度参数Ω2.发现Li+共掺杂有助于提高GdTaO4:Eu3+的发光强度,当x=0.06和0.10时,612 nm处的发光强度分别被提升了1.7倍和1.5倍.发光增加的原因是因为Li+的助熔剂效应有效提高了GdTaO4材料的结品性能,并抑制了Cd2O3和Ta2O5杂相的产生,而非所推测的掺Li+引起了配位场对称性降低,从而导致宇称禁戒的放宽.此时Gd0.92-xLixTaO4:Eu3+0.08材料不仪结晶性能较好,而且Gd2O3和Ta2O5杂相也相对较少,故而发光增强最为明显.     

自受激拉曼晶体Nd3+:SrMoO4的光谱性质研究

通过拉曼散射光谱，吸收光谱，荧光发射寿命和808 nm LD激发下的红外荧光光谱的实验测量，系统研究了Nd³⁺:SrMoO₄晶体的自受激拉曼光谱性质.分析指认了拉曼散射光谱中各拉曼峰所对应的晶格振动模式，得出了其SRS活性最强的声子频率约为898 cm^-1，对应于(MoO^2-₄)离子团的完全对称光学伸缩振动A_g模；通过J-O理论对晶体的吸收谱进行了全面的光谱参数计算，得出⁴F_3/2→⁴I_11/2跃迁的积分发射截面达0.57×10^-18 cm²，自发辐射概率为141.06 s^-1；同时，实验测得该跃迁的荧光发射寿命约为0.2 ms.最后，结合808 nm LD激发下的红外波段荧光光谱，论证了SrMoO₄晶体中Nd³⁺离子1068 nm发射通过拉曼频移获得1180 nm一级斯托克斯激光发射的可能性，为Nd³⁺:SrMoO₄晶体的自受激拉曼激光器研究提供了理论依据. 关键词： 3+离子')" href="#">d³⁺离子 4 晶体')" href="#">SrMoO₄ 晶体 自受激拉曼散射     

掺杂分子晶体NH_（4－x）D_xNO_3相变中的分形行为──NO_3~－u_1、u_4振动模临界态拉曼峰强的研究

掺杂分子晶体ＮＨ＿（４－ｘ）Ｄ＿ｘＮＯ＿３相变中的分形行为──ＮＯ_３~－ｕ＿１、ｕ＿４振动模临界态拉曼峰强的研究马树国，吴国祯（清华大学物理系北京１０００８４）ＴｈｅＦｒａｃｔａｌＩｎｔｅｒｐｒｅｔａｔｉｏｎｏｆｔｈｅＰｈａｓｅＴｒａｓｉｔｉｏｎｏｆ...     

Li^+掺杂对SrLu_2O_4∶Ho^(3+)/Yb^(3+)荧光粉上转换发光性能的影响EI北大核心CSCD

采用高温固相反应法制备了一系列Li^+掺杂的SrLu_2O_4∶Ho^(3+)/Yb^(3+)荧光粉。Li^+掺杂并没有改变样品原有的斜方晶系结构,Li^+离子能够以替代掺杂和间隙掺杂的方式进入主晶格。适当的Li^+掺杂可以改善样品的团聚现象,颗粒粒径约为3μm。Li^+的引入还可减少高声子能量杂质基团(OH^-,CO_3^(2-)),从而减少荧光猝灭中心,增强发光。在980nm激光照射下,样品发出强烈的绿光和很弱的红光,分别归因于Ho^(3+)的~5F_4,~5S_2→~5I_8和~5F_5→~5I_8跃迁。与SrLu_2O_4∶Ho^(3+)/Yb^(3+)样品相比,Li^+的掺杂使得上转换发光强度明显增强,其原因是Li^+可以修饰Ho^(3+)周围局域晶体场的对称性。与其他碱金属离子掺杂相比,Li^+半径最小、电负性最强,导致发光强度增强最多。抽运依赖分析结果表明,绿光与红光发射均为双光子过程。     

Pressure effect on the Raman and photoluminescence spectra of Eu3+-doped Na2Ti6O13 nanorods

Eu³⁺-doped Na₂Ti₆O₁₃ (Na₂Ti₆O₁₃:Eu) nanorods with diameters of 30 nm and lengths 400 nm were synthesized by hydrothermal and heat treatment methods. Raman spectra at ambient conditions indicated a pure monoclinic phase (space group C2/m) of the nanorods. The relations between structural and optical properties of Na₂Ti₆O₁₃:Eu nanorods under high pressures were obtained by photoluminescence and Raman spectra. Two structural transition points at 1.39 and 15.48 GPa were observed when the samples were pressurized. The first transition point was attributed to the crystalline structural distortion. The later transition point was the result of pressure-induced amorphization, and the high-density amorphous (HDA) phase formed after 15.48 GPa was structurally related to the monoclinic baddeleyite structured TiO₂ (P2₁/c). However, the site symmetry of the local environment around the Eu³⁺ ions in Na₂Ti₆O₁₃ increased with the rising pressure. These above results indicate the occurrence of short-range order for the local asymmetry around the Eu³⁺ ions and long-range disorder for the crystalline structure of Na₂Ti₆O₁₃:Eu nanorods by applying pressure. After releasing the pressure from 22.74 GPa, the HDA phase is transformed to low-density amorphous form, which is attributed to be structurally related to the α-PbO₂-type TiO₂.     

A2( MoO4)3(A=Al,Cr,Fe)结构与相变的Raman光谱研究

用XRD、Raman光谱和DSC研究了Al2 (MoO4)3、Cr2( MoO4)3和Fe2 (MoO4)3的结构与相变.Al2(MoO4)3、Cr2 (MoO4)3和Fe2 (MoO4)3在室温下为单斜相,分别在483 K、673 K和783 K附近转变为正交相.发现MO4四面体的对称和反对称伸缩振动模的频率和相对强...     

Manifestations of Phase Transitions and the Thermooptical-Memory Effect in the Absorption Spectra of (N(CH<Subscript>3</Subscript>)<Subscript>4</Subscript>)<Subscript>2</Subscript>CuCl<Subscript>4</Subscript> Crystals

The manifestations of phase transitions and the spatial modulation of the structure of the (N(CH₃)₄)₂CuCl₄ crystal in its absorption spectra have been investigated. It has been established that the thermooptical-memory effect manifesting itself in the absorption spectra of this crystal entirely corresponds to the model of ordering of defects and impurities in a sample with a modulated structure. It is shown that, as a result of stabilization of the crystal studied in the incommensurate phase, its symmetry and the symmetry of the metal-halogen complex in it lower depending on the defect wave. This manifests itself as a marked shift of the intraionic-absorption bands and an increase in their intensity. __________ Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 72, No. 3, pp. 386–390, May–June, 2005.     

High‐pressure studies of the micro‐Raman spectra of iron cyanide complexes: Prussian blue (Fe4[Fe(CN)6]3), potassium ferricyanide (K3[Fe(CN)6]), and sodium nitroprusside (Na2[Fe(CN)5(NO)]·2H2O)

The pressure dependences of the peaks observed in the micro‐Raman spectra of Prussian blue (Fe₄[Fe(CN)₆]₃), potassium ferricyanide (K₃[Fe(CN)₆]), and sodium nitroprusside (Na₂[Fe(CN)₅(NO)]·2H₂O) have been measured up to 5.0 GPa. The vibrational modes of Prussian blue appearing at 201 and 365 cm⁻¹ show negative dν/dP values and Grüneisen parameters and are assigned to the transverse bending modes of the Fe C N Fe linkage which can contribute to a negative thermal expansion behavior. A phase transition occurring between 2.0 and 2.8 GPa in potassium ferricyanide is shown by changes in the spectral region 150–700 cm⁻¹. In the spectra of the nitroprusside ion, there are strong interactions between the FeN stretching mode and the FeNO bending and the axial CN stretching modes. The pressure dependence of the NO stretching vibration is positive, 5.6 cm⁻¹ GPa⁻¹, in contrast to the negative behavior in the iron(II)‐meso‐tetraphenyl porphyrinate complex. Copyright © 2011 John Wiley & Sons, Ltd.     

N^＋（N=Li,Na,K）对发光材料M3（M=Ca,Sr,Ba）Y2（BO3）4：Eu^3＋光谱的影响

采用高温固相反应方法在空气中制备了M3(M=Ca,Sr,Ba)Y2(BO3)4∶Eu3 红色发光材料,测量结果显示,材料的主发射峰均位于613 nm处,监测613 nm发射峰时,所得材料的激发光谱相同。研究了Li ,Na 和K 对M3(M=Ca,Sr,Ba)Y2(BO3)4∶Eu3 材料激发与发射光谱的影响,结果显示,加入Li ,Na 和K 后,M3(M=Ca,Sr,Ba)Y2(BO3)4∶Eu3 材料的激发与发射光谱的峰值位置并不发生变化,但材料的激发与发射光谱的峰值强度均得到了不同程度的增强。在Li ,Na 和K 掺入浓度相同的条件下,研究发现,与加入Na 和K 时相比,加入Li 时,M3(M=Ca,Sr,Ba)Y2(BO3)4∶Eu3 材料的激发与发射光谱的峰值增强效果最明显。进而研究了Sr3Y2(BO3)4∶Eu3 材料发射峰强度随Li 掺杂浓度的变化情况,结果表明,随着Li 掺杂浓度的增大,Sr3Y2(BO3)4∶Eu3 材料发射峰强度先增大后减小,在Li 浓度为5 mol%时到达峰值,约为未掺杂时的两倍。     

A nuclear magnetic resonance study of the phase transitions and electric quadrupole Raman processes of M5H3(SO4)4·H2O (M=Na, K, Rb, and Cs) single crystals

The spin–lattice relaxation times and spin–spin relaxation times for ¹H and M in M₅H₃(SO₄)₄·H₂O (M=Na, K, Rb, and Cs) single crystals grown using the slow-evaporation method were measured as functions of temperature. Two kinds of protons were identified in the M₅H₃(SO₄)₄·H₂O structure: acid protons and water protons. Our experimental results show that the acid and water protons in Cs₅H₃(SO₄)₄·H₂O are involved in phase transitions of this crystal, whereas neither type of proton is involved in the phase transitions of the other three crystal type (M₅H₃(SO₄)₄·H₂O; M=Na, K, and Rb). Moreover, the relaxation times for the M (=Na, K, and Rb) nuclei in these crystals were found to decrease with increasing temperature and can be described with (k=2). The T₁ results for M (=Na, K, and Rb) in M₅H₃(SO₄)₄·H₂O crystals can be explained in terms of a relaxation mechanism in which the lattice vibrations are coupled to the nuclear electric quadrupole moments.