Thickness Effect on (La_(0.26)Bi_(0.74))_2Ti_4O_(11) Thin-Film Composition and Electrical Properties

Highly oriented(00l)(La_(0.26)Bi_(0.74))_2Ti_4O_(11 )thin films are deposited on(100) SrTiO_(3 )substrates using the pulsed laser deposition technique.The grains form a texture of bar-like arrays along Sr Ti O_3110directions for the film thickness above 350 nm,in contrast to spherical grains for the reduced film thickness below 220 nm.X-ray diffraction patterns show that the highly ordered bar-like grains are the ensemble of two lattice-matched monoclinic(La,Bi)_4Ti_3O_(12 )and TiO_(2 )components above a critical film thickness.Otherwise,the phase decomposes into the random mixture of Bi_2Ti_2O_(7 )and Bi_4Ti_3O_(4 )spherical grains in thinner films.The critical thickness can increase up to 440 nm as the films are deposited on LaNiO_3-buffered SrTiO_(3 )substrates.The electrical measurements show the dielectric enhancement of the multi-components,and comprehensive charge injection into interfacial traps between(La,Bi)_4Ti_3O_(12 )and TiO_(2 )components occurs under the application of a threshold voltage for the realization of high-charge storage.     

Polarization Mechanism in Filled Tungsten Bronze Ba_4Eu_2Ti_4Nb_6O_(30) with Pinched P-E Hysteresis Loops

Pinched P-E hysteresis loops have been observed in filled tungsten bronze Ba_4Eu_2Ti_4Nb_6O_(30),indicating the presence of novel polarization mechanisms.We investigate the evolution of polar order in filled tungsten bronze Ba_4Eu_2Ti_4Nb_6O_(30),together with its dielectric properties over a wide temperature range,from 50 K to 773 K.The temperature dependences of the dielectric properties exhibit two low-temperature dielectric relaxations,at around 300 K(P1),and 100 K(P2),and a high temperature peak at 588 K with no frequency dispersion,indicating the ferroelectric transition temperature T_c.Pinched P-E loops are observed in the temperature range between the low temperature relaxation at P1,and the ferroelectric transition.On cooling,the pinched P-E hysteresis loops open gradually,with increasing remnant polarization(Pr).Two pairs of reversal electric fields indicate two types of polar reversal mechanisms,with an activated energy of 1.41 eV(E_1),and 0.94 eV(E_2),respectively.One corresponds to the field-induced transition from a nonpolar to a polar state,which dominates at a high temperature close to T_c,while the other relates to the reversal of ferroelectric domains which stabilize gradually on cooling.At temperatures below 300 K,the polarization exhibits an evident decrease,probably related to the disruption of the polar order due to the dielectric relaxation at P1.     

La,V共掺杂的Bi_4Ti_3O_(12)铁电薄膜的溶胶-凝胶法制备及性能测试

采用溶胶-凝胶(sol-gel)工艺在Pt/TiO2/SiO2/p-Si(100)衬底上制备出Bi4Ti3O12(BIT)和Bi3.25La0.75Ti2.97V0.03O12(BLTV)铁电薄膜,研究了La,V共掺杂对BIT薄膜的晶体结构和电学性能的影响.BIT薄膜为c轴择优取向,BLTV薄膜为随机取向,拉曼光谱分析表明V掺杂降低了TiO6(或VO6)八面体的对称性,也增强了Ti—O键(或V—O键)杂化.BLTV薄膜的剩余极化Pr为25.4μC/cm2,远大于BIT薄膜的9.2μC/cm2,表现出良好的铁电性能.疲劳、漏电流测试显示BLTV薄膜具有优良的抗疲劳特性和漏电流特性,表明La,V共掺杂能有效地降低薄膜中的氧空位.     

Bi1.8Nd0.2Ti4O11的温致及压致软模相变研究

 采用背用散射的方法，测量了Bi_1.8Nd_0.2Ti₄O₁₁的拉曼光谱。实验结果表明，该掺杂样品发生温致和压致软模相变的温度和压力分别为200 ℃和3.35 GPa。文中讨论了相变点移动的原因及高频声子模随温度和压力的变化。     

Bi4-xLaxTi3O12-SrBi4Ti4O15,共生结构铁电材料拉曼光谱研究

在常温下，对La掺杂共生结构铁电陶瓷Bi_4-xLa_xTi_3O_12-SrBi_4-yLayTi_4O_15［BLT-SBLT(x+y),x+y= 0.00, 0.25,0.50,0.75,1.00,1.25,1.50］进行了拉曼光谱研究.结果表明，在掺杂量低于0.50时，La只取代类钙钛矿层中的Bi，当掺杂 量高于0.50后，部分La开始进入(Bi_2O_2)^2+层. La取代(Bi_2O_2)^2+层中的部分Bi以后，(Bi_2O_2)^2+层结构发生变化 ，原有的绝缘层和空间电荷库的作用减弱，导致材料剩余极化下降. La掺杂量增至1.50时，样品出现弛豫铁电性，这与30cm^-1以下模的软化相对应，说明La掺杂可引起材料 的结构相变. 关键词： Bi4-xLaxTi3O12-SrBi4Ti4O15 La掺杂 声子模 拉曼频移     

Low temperature ferromagnetism in CaCu_3Ti_4O_(12)

The low-temperature magnetic order behaviors of perovskite oxide CaCu_3 Ti_4 O_(12)(CCTO) ceramics prepared by different methods are discussed.X-ray diffraction,scanning electron microscope,x-ray photoelectron spectroscopy,and direct current(DC) magnetization are used to characterize the structures,microscopic morphologies,valence states,and magnetic properties of the samples.The results show that the magnetic behaviors of CCTO ceramics are very sensitive to the preparation process.The quenched CCTO ceramic and CCTO powders grown in a molten salt crystal,which contain much more oxygen vacancies and Ti~(3+),show the coexistence of weak ferromagnetic order and antiferromagnetic order below the Neel temperature.It suggests that the bound magnetopolaron formed by oxygen vacancies and Ti~(3+) ion composite defects are responsible for the weak ferromagnetic order at low temperature.     

Bi_（2－x）Fe_xTi_4O_（11）体系的拉曼光谱研究

Ｂｉ＿（２－ｘ）Ｆｅ＿ｘＴｉ＿４Ｏ＿（１１）体系的拉曼光谱研究赵明旭，孟进芳（长春教育学院物理系长春１３００６１）（河南大学物理系开封４７５００１）ＩｎｖｅｓｔｉｇａｔｉｏｎｓｏｆＲａｍａｎＳｐｃｔｒａｉｎＢｉ＿（２－ｘ）Ｆｅ＿ｘＴｉ＿４Ｏ＿（１１）...     

Sb_xBi_(2-x)Ti_4O_(11)体系的拉曼光谱及软模行为研究

本文合成出了系列样品Sb_xBi_(2-x)Ti_4O_(11),得到了它们在常温常压下的拉曼光谱。实验结果发现:体系在x=0.4和1.2处经历了两次相转变,且相变与“软模”随Sb~(+3)的浓度变化有关。     

Sr2Bi4Ti5O18的压致结构相变

 使用4∶1的甲醇-乙醇混合液作传压介质，利用金刚石对顶砧装置（DAC），研究了层状铁电体Sr₂Bi₄Ti₅O₁₈的在位高压拉曼光谱和压致结构相变（0～27 GPa）。发现在8.31 GPa，Sr₂Bi₄Ti₅O₁₈经历了一次结构相交。在23.13 GPa以上，Sr₂Bi₄Ti₅O₁₈似乎出现了压致非晶相交的先兆。并使用内模方法对Sr₂Bi₄Ti₅O₁₈的内模进行了指认。     

Improved thermoelectric performance in p-type Bi_(0.48)Sb_(1.52)Te_3 bulk material by adding MnSb_2Se_4

Bismuth telluride(Bi_2Te_3) based alloys, such as p-type Bi_(0.5)Sb_(1.5)Te_3, have been leading candidates for near room temperature thermoelectric applications. In this study, Bi_(0.48)Sb_(1.52)Te_3 bulk materials with MnSb_2Se_4 were prepared using high-energy ball milling and spark plasma sintering(SPS) process. The addition of MnSb_2Se_4 to Bi_(0.48)Sb_(1.52)Te_3 increased the hole concentration while slightly decreasing the Seebeck coefficient, thus optimising the electrical transport properties of the bulk material. In addition, the second phases of MnSb_2Se_4 and Bi_(0.48)Sb_(1.52)Te_3 were observed in the Bi_(0.48)Sb_(1.52)Te_3 matrix. The nanoparticles in the semi-coherent second phase of MnSb_2Se_4 behaved as scattering centres for phonons,yielding a reduction in the lattice thermal conductivity. Substantial enhancement of the figure of merit, ZT, has been achieved for Bi_(0.48)Sb_(1.52)Te_3 by adding an Mn_(0.8)Cu_(0.2)Sb_2Se_4(2mol%) sample, for a wide range of temperatures, with a peak value of 1.43 at 375 K, corresponding to ~40% improvement over its Bi_(0.48)Sb_(1.52)Te_3 counterpart. Such enhancement of the thermoelectric(TE) performance of p-type Bi_2Te_3 based materials is believed to be advantageous for practical applications.     

从自旋冰到自旋液态的渡越——结构与磁性质的演化

使用固相反应法得到了Ho_2-xTb_xTi₂O₇（x=0,05,1,15,2）系列多晶样品.X射线衍射（XRD）实验与2K到300K温度区间的直流磁化率测量结果显示,随着Tb即是x的增加,体系由自旋冰Ho₂Ti₂O₇向自旋液Tb₂Ti₂O_{7关键词： 自旋冰 自旋液体 自旋阻挫 晶格结构}     

Magnetic field aligned orderly arrangement of Fe_3O_4 nanoparticles in CS/PVA/Fe_3O_4 membranes

The CS/PVA/Fe_3O_4 nanocomposite membranes with chainlike arrangement of Fe_3O_4 nanoparticles are prepared by a magnetic-field-assisted solution casting method. The aim of this work is to investigate the relationship between the microstructure of the magnetic anisotropic CS/PVA/Fe_3O_4 membrane and the evolved macroscopic physicochemical property. With the same doping content, the relative crystallinity of CS/PVA/Fe_3O_4-M is lower than that of CS/PVA/Fe_3O_4.The Fourier transform infrared spectroscopy(FT-TR) measurements indicate that there is no chemical bonding between polymer molecule and Fe_3O_4 nanoparticle. The Fe_3O_4 nanoparticles in CS/PVA/Fe_3O_4 and CS/PVA/Fe_3O_4-M are wrapped by the chains of CS/PVA, which is also confirmed by scanning electron microscopy(SEM) and x-ray diffraction(XRD)analysis. The saturation magnetization value of CS/PVA/Fe_3O_4-M obviously increases compared with that of non-magnetic aligned membrane, meanwhile the transmittance decreases in the UV-visible region. The o-Ps lifetime distribution provides information about the free-volume nanoholes present in the amorphous region. It is suggested that the microstructure of CS/PVA/Fe_3O_4 membrane can be modified in its curing process under a magnetic field, which could affect the magnetic properties and the transmittance of nanocomposite membrane. In brief, a full understanding of the relationship between the microstructure and the macroscopic property of CS/PVA/Fe_3O_4 nanocomposite plays a vital role in exploring and designing the novel multifunctional materials.     

Site Preference of Se and Te in Bi_2Se_(3-x)Te_x Thin Films

The ternary topological insulators Bi₂Se_3-xTe_x have attracted a great deal of attention due to their exotic physical and chemical properties.While most of the studies focus on the properties of these ternary TIs,limited research was performed to investigate the dynamic atomic stack of its crystal structure.We prepared highquality Bi₂Se_3-xTe_x thin films on Ga As(111)B substrates using molecular beam epitaxy,characterized with Raman...     

Substitution priority of Eu~(2+) in multi-cation compound Sr_(0.8)Ca_(0.2)Al_2Si_2O_8 and energy transfer

A blue phosphor was obtained by doping Eu~(2+)into a multi-cation host Sr_(0.8)Ca_(0.2)Al_2Si_2O_8 through high temperature solid state reaction.The emission spectra show a continuous red-shift behavior from 413 nm to 435 nm with Eu~(2+)concentration increasing.The substitution priority of Eu~(2+)in Sr_(0.8)Ca_(0.2)Al_2Si_2O_8 was investigated via x-ray diffraction(XRD)and temperature properties in detail:the Ca~(2+)ions are preferentially substituted by Eu~(2+)at lower doping,and with the Eu~(2+)concentration increasing,the probability of substitution for Sr~(2+)is greater than that of replacing Ca~(2+).Accordingly,we propose the underlying method of thermal property to determine the substitution of Eu~(2+)in the multi-cation hosts.Moreover,the abnormal increase of emission intensity with increasing temperature was studied by the thermoluminescence spectra.The energy transfer mechanism between the Eu~(2+)ions occupying different cation sites was studied by the lifetime decay curves.A series of warm white light emitting diodes were successfully fabricated using the blue phosphors Sr~+_(0.8)Ca_(0.2)Al_2Si_2O_8:Eu~2 with commercial red phosphor (CaSr)SiAlN_3:Eu~(2+)and green phosphor(Y Lu)_3Al_5O_(12):Ce~(3+),and the luminescent efficiency can reach 45 lm/W.     

Bi_2Ti_2O_7/Si薄膜的制备及C-V特性研究

采用化学溶液分解法 (CSD)在Si衬底上制备了Bi2 Ti2 O7薄膜 .X射线双晶衍射和原子力显微镜检测表明 ,所制备的薄膜主要为Bi2 Ti2 O7相的多晶材料 .同时还研究了Au Bi2 Ti2 O7 n Si(10 0 )结构的电容 电压 (C V)特性 ,结果表明 ,在Bi2 Ti2 O7薄膜中同时存在固定的与可移动的负电荷 ,可移动的负电荷导致了C V曲线的回线效应     

The Complex Magnetism in the Breathing Pyrochlore LiIn(Cr_(1-x)Rh_x)_4O_8

We perform a detailed investigation of the new 'breathing' pyrochlore compound LiInCr_4O_8 through Rh substitution with measurements of magnetic susceptibility,specific heat,and x-ray powder diffraction.The antiferromagnetic phase of LiInCr_4O_8 is found to be slowly suppressed with increasing Rh,up to the critical concentration of x=0.1 where the antiferromagnetic phase is still observed with the peak in specific heat T_p=12.5K,slightly lower than T_p=14.3 K for the x=0 compound.From the measurements of magnetization we also uncover evidence that substitution increases the amount of frustration.Comparisons are made with the LiGa_yIn_(1-y)Cr_4O_8system as well as other frustrated pyrochlore-related materials and comparable amounts of frustration are found.The results of this work show that the engineered breathing pyrochlores present an important method to further understand the complex magnetism in frustrated systems.     

SrAl_2O_4∶Eu,Dy纳米材料与体材料的光电特性研究

用溶胶-凝胶自燃烧法和高温固相法分别制备了纳米和体相SrAl_2O_4:Eu,Dy长余辉磷光体.用X射线衍射对晶体结构进行了表征,用Keithley 2410对材料在有无光照条件下的电流-电压特性进行了分析,同时还测量了样品的真空紫外激发光谱.光照使材料的电流增强,说明至少有部分电子经光照后被激发到导带;纳米材料真空紫外激发光谱发生蓝移,说明纳米材料的禁带宽度要大于体材料的禁带宽度,相同电压下纳米材料的电流小于体材料的电流.     

Pu(100)表面吸附CO2的密度泛函研究

采用广义梯度密度泛函理论的改进Perdew-Burke-Ernzerh方法结合周期性层晶模型,研究了CO₂分子在Pu（100）面上的吸附和解离.吸附能和几何构型的计算表明,CO₂以穴位C4O4构型吸附最为有利,吸附能为1.48 eV.布居分析和态密度分析表明,CO₂与Pu表面相互作用的本质主要是CO₂分子的杂化轨道2π_μ与Pu5f,Pu6d,Pu7s轨道通过强电子转移和弱重叠杂化的方式相互作用而生成了新的化学键.计算的CO₂→CO+O解离能垒为0.66 eV,解离吸附能为2.65 eV, 表明在一定热激活条件下CO₂分子倾向于发生解离性吸附.O₂,H₂,CO和CO₂在Pu （100）面吸附的比较分析表明,较低温度下的吸附强度顺序依次为O₂,CO,CO₂,H₂;较高温度下的吸附强度顺序依次为O₂,CO₂,CO,H₂. 关键词： 密度泛函理论 Pu （100） 2')" href="#">CO₂ 吸附和解离     

K_2C_2O_4,Mg(NO_3)_2和Na_2S_2O_3过饱和水溶液瑞利弛豫的不连续行为

本文用瑞利散射强度相关的方法求得了K_2C_2O_4,Mg(NO_3)_2和Na_2S_2O_3水溶液的弛豫时间常数。结果表明当达到过饱和态时,弛豫时间常数有不连续增大的趋势。连同过去关于NH_4H_2PO_4的报导,显示这是过饱和体系的一个共同特征。此弛豫时间常数因此可以做为标度从不饱和相至饱和相转变的有序度参数。     

Ca~(2+)离子替代对Sr_4Al_(14)O_(25):Eu~(2+),Dy~(3+)结构和发光性能的影响

采用高温固相反应按化学式Sr4-xCaxAl14O25:Eu2+,Dy3+(x=0,0.8,1.6,2.4,3.2,4)配比原料,合成长余辉发光材料.X射线衍射分析表明当x2.4时,产物物相均为Sr4Al14O25正交结构;当x2.4时,产物物相转变为CaAl4O7单斜结构.对掺Ca量不同,但结构仍保持Sr4Al14O25的样品采用360nm激光照射,发射光谱表明样品发光均由以Eu2+为发光中心的电子4f65d→4f7跃迁所致,并且随着Ca掺入量的增加,样品发射光谱峰位逐渐蓝移.这是由于Ca2+取代Sr2+位置后,导致晶格收缩,影响Eu2+的5d能级劈裂情况,从而影响电子4f65d→4f7跃迁.余辉衰减检测和热释光谱分析发现,不同Ca掺入量的样品余辉衰减快慢不同,是由于其中存在的陷阱能级深度不同,且陷阱能级越深,其余辉时间越长.