Ag／La0.67Sr0.33MnO3/Pt异质结构的电阻开关特性

采用脉冲激光沉积技术在Pt／Ti／SiO2／Si（100）衬底上制备出多晶La0.67Sr0.33MnO3（LSMO）薄膜,对其电脉冲致非挥发可逆电阻开关特性进行研究．结果表明,Ag/LSMO／Pt结构具有明显的室温电脉冲诱发电阻开关特性,且在宽电压脉冲作用下表现出较低的开关电压和较快的变阻饱和速度．由此可见,总脉冲能量或电荷（电流作用）为该结构的电阻开关效应提供驱动力．对Ag／LsMO／Pt结构进行了耐久性测试,表明该结构具有良好的疲劳特性与保持特性,可应用于新型不挥发存储器、传感器及可变电阻等电子元器件的研制     

La0.67 Sr0.33 MnO3外延薄膜的电脉冲诱发可逆变阻效应

采用脉冲激光沉积技术在SrTiO3,(001)单晶衬底上制备出钙钛矿结构La0.67 Sr0.33 MnO3,(LSMO)外延薄膜,通过X射线衍射仪和原子力显微镜表征其晶体取向与表面形貌,并对Ag-LSMO结构的室温电脉冲诱发可逆变阻效应进行研究.结果表明,在±4V、50ns对称脉冲作用下,LSMO膜层电阻发生高低转变,且变阻范围随脉冲幅值电压、脉冲宽度、脉冲数日等参数的变化而变化.该效应表现出良好的疲劳特性与非挥发存储特性,有望应用于新型不挥发存储器、传感器、可变电阻等电子元器件的研制.     

La0.67Sr0.33MnO3中Bi的掺杂效应

将Bi2O3掺杂到用溶胶—凝胶法制备的La0.6Sr0．33MnO3(LSMO)微粉中,XRD测量结果证实有过量的Bi析出。随着Bi掺杂量的增加,LSMO／(Bi2O3)x/2材料电阻率发生明显变化,在x=(0—0．10)摩尔比的掺杂范围内,电阻率先上升后突然下降。当X=0．1时,电阻率比未掺杂样品下降了一个数量级。Bi掺杂对低温和室温磁电阻有着完全不同的影响。低温下,随掺杂量增加,磁电阻下降;室温下Bi的微量掺杂可以使磁电阻增大,掺入x=0.03Bi使室温磁电阻由-4.4％提高到-5．6％。     

Dy和Yb部分替代La0.67Ca0.33MnO3中的La的影响

用Dy和Yb部分替代La0.67Ca0.33MnO3中的La使材料的居里温度单调下降，掺Dy使材料的相变温度单调下降，峰值电阻率迅速增大，磁电阻比急剧增大，掺入13％（原子分数）的Dy可使材料的最大磁电阻比增大近40倍，而掺Yb对磁电阻的影响要小得多，用自旋团簇理论可以解释庞磁电阻的形成。     

Ti掺杂对La0.67Ba0.33MnO3磁性和磁电阻影响

系统地研究了Ti掺杂对La0.67Ba0．33MnO3颗粒材料磁性、电性和磁电阻效应的影响，随着Ti含量的增加，材料的磁化强度和居里温度快速下降，电阻率急剧增大，电阻率的峰值逐渐向低温移动。Ti的掺杂对材料低温下低场磁电阻影响不大，主要是显著提高了材料的本征磁电阻。1％的Ti掺杂使材料的室温磁电阻得到显著增强，1T磁场下，室温磁电阻达到-8．4％，比未掺杂的La0.67Ba0．33MnO3材料增强了50％。     

Irreversible Colossal Magnetoresistance in La0.58Dy0.09Ca0.33MnO3

The representative sample La0.58Dy0.09Ca0.33MnO3 of Dy doped La0.67Ca0.33MnO3 rare-earth manganites was investigated.The most important effect of Dy doping is to introducethe magnetoimpurity and form the spin clusters which induce dramatically large CMR in Lao.58Dyo.09Cao.33MnO3. The fitting results of field-induced resistivity decrease to the Brillouin function indicate that the CMR is caused by the spin dependent hopping between spin clusters. It is the magnetic field that reduces the size of spin clusters and induces a field-induced irreversible CMR behaviour.     

不同厚度的La2/3Sr1/3MnO3多晶薄膜输运性质研究

运用磁控溅射的方法,在表面氧化的Si(100)基片上制备了一系列不同厚度的La2/3Sri/3MnO3多晶薄膜.根据对输运的研究,发现存在一个厚度73nm,当t＞73nm的时候,薄膜呈现出与块材类似的输运特点,而当t＜73nm的时候,薄膜的电阻太大以至于薄膜的金属-绝缘体转变温度(Tp)变得不可测量.X射线衍射(XRD)结果显示:在t=73nm附近存在一个结构的转变.这表明La2/3Sr1/3MnO3不同厚度多晶薄膜的输运性质的不同或许来自结构的转变.     

La0.67Ca0.33-0.5xLixMnO3多晶陶瓷结构及电学性能研究

用溶胶-凝胶法制备La0.57Ca0.33-0.5xLixMnO3(x=0.00,0.05,0.10,0.20)多晶陶瓷,用XRD分析多晶陶瓷的晶体结构,用SEM对多晶陶瓷的微观形貌进行分析,用标准四探针法测量电阻率-温度关系.结果表明,随着Li掺杂量的增加,所有样品均为斜方晶系,晶胞体积不断减小,金属-绝缘体转变温度(Yp)降低,电阻率不断增加,电阻率温度系数(TCR)不断减小.低温区域(T＜TP)的电阻率数据可以用ρ(T)=ρ0+ρ2T2 +ρ4.5T4.5进行拟合;高温区域(T＞TP)的电阻率数据可以用小极化子跃迁(SPH)模型和变程跳跃(VRH)模型进行拟合.整个温度区域(100～300 K)可以使用渗透模型对电阻率进行拟合.从拟合数据可知极化子激活能Ea随Li掺杂量的增加而增大,这是由于Li的加入减小了Mn3+-O2--Mn4+的键角,增大了有效带宽的间隙,因此也减弱了双交换作用,增大了电阻率.     

烧结温度对La0.67Ca0.33-xSrxMnO3结构及电学性能的影响

采用传统固相反应法合成了双掺杂La_0.67Ca_0.33-xSr_xMnO₃(x=0, 0.05, 0.15)粉体, 研究了烧结温度对La_0.67Ca_0.33-xSr_xMnO₃(x=0, 0.05, 0.15)结构、微观形貌和金属-绝缘体相转变温度的影响规律。结果表明: 烧结温度的升高对微观形貌及结构影响较小, 双掺杂有效改善了材料体系的相转变温度。当烧结温度为1400℃, 掺杂量x=0增加至x=0.05时, 材料体系为正交相, 相转变温度从-20℃升高至6℃。掺杂量继续增加至x=0.15, 材料体系从正交相转变为六方相, 相转变温度升高至17℃。当掺杂量相同时, 相转变温度随烧结温度的升高而升高。具有上述智能相变特性的材料体系可以作为长寿命卫星主动热控技术的重要候选材料。     

高温燃料电池阴极材料La（Sr）MnO3的电导性能研究

用固相合成法合成了（Ｌａ１－ｘＳｒｘ）１－ｙＭｎＯ３（ｘ＝０～５，ｙ＝０～０．１）单纯相化合物。在空气中用直流四探针法测定了各组成的电导率。测试温度范围为１００～９５０℃。其中（Ｌａ０．７Ｓｒ０．３）０．９５ＭｎＯ３具有最大的电导率。讨论了Ｌａ（Ｓｒ）ＭｎＯ３的电导机理。     

Nb5+的掺杂引起La0.67Sr0.33MnO3增强的磁电阻效应

将Nb2O5掺杂到用溶胶-凝胶法制备的La0.67Sr0.33MnO3(LSMO)微粉中,XRD测量结果表明所有样品均为单相菱面结构.随着Nb5 掺杂量的增加,材料电阻率发生显著变化.在x=0.06的掺杂样品中得到最高为1110Ω·cm电阻率(x是掺入的Nb离子与母体材料的摩尔比),比LSMO高5个数量级,这是由于晶界处以及颗粒内部增加的自旋相关的散射和隧穿效应所致.Nb5 离子的掺杂使样品的低场磁电阻(LFMR)和高场磁电阻(HFMR)效应都有所增强.77K下,0.1和1T磁场下在x=0.07样品中分别得到25%和42%的磁电阻效应,分别是LSMO样品的2倍和1.7倍.室温下x=0.03样品的磁电阻最大,为7%.其中,LFMR来源于颗粒晶界处电子的自旋相关隧穿及散射作用,而HFMR来源于表面层的自旋非共线结构.     

Magnetodielectric properties of nano-crystalline BaZr0.15Ti0.85O3/La0.67Sr0.33MnO3 thin film heterostructures

The paper discuses synthesis of La_0.67Sr_0.33MnO₃ and BaZr_0.15Ti_0.85O₃ thin film heterostructures using modified Pechini method (citrate gel) and spin coating technique. The XRD spectra are determined for confirmation of the crystal structure and phase formation of thin film composites. The paper presents variation of real and imaginary parts of dielectric constant ε′, ε″ and tan δ as function of frequency between 100 Hz and 1 MHz and applied magnetic field up to 0.6 T. The paper, also discuses the effect of magnetic field on AC conductivity. The observed variation of magnetocapacitance and impedance spectra are analyzed in terms of a possible equivalent circuit model. The present analysis shows that the method of impedance spectra could be used to separate out the possible contributions to the magnetodielectric effect.     

Magnetic Properties of Interacting La0.67Sr0.33MnO3 Nanoparticles

Magnetic nanoparticles of La_0.67Sr_0.33MnO₃ (LSMO) with mean particle sizes of 13, 16, 18, and 21 nm were prepared by the sol?Cgel method. The samples were characterized by X-ray diffraction (XRD) using Rietveld refinement and transmission electron microscope (TEM). Fourier transform infrared (FTIR) transmission spectroscopy revealed that stretching and bending modes are influenced by annealing temperature. Dc magnetization versus magnetic field of the samples was carried out at room temperature. Magnetic dynamics of the samples was studied by the measurement of ac magnetic susceptibility versus temperature at different frequencies and ac magnetic fields. A frequency-dependent peak was observed in ac magnetic susceptibility versus temperature which is well described by Vogel?CFulcher and critical slowing down laws, and empirical $c_{1} = \frac{\Delta T_{f}}{T_{f}\Delta (\log _{10}f)}$ and $c_{2} = \frac{T_{f} -T_{0}}{T_{f}}$ parameters. By fitting the experimental data with Vogel?CFulcher magnetic anisotropy energy and an effective magnetic anisotropy constant have been estimated. The obtained values support the presence of strong interaction between magnetic nanoparticles of LSMO.     

La0.67Sr0.33MnO3中Ag-Ti的掺杂效应

将La0.67Sr0.33MnO3（LSMO）、Ag2O及TiO2粉混合经高温烧结后制备了钙钛矿相/xAg两相复合体系（x是Ag与钙钛矿材料的物质的量比）,系统地研究了Ag-Ti的共掺杂对LSMO电性和磁电阻效应的影响.0.07摩尔比Ti4＋离子的B位掺杂使LSMO的居里温度降至室温.Ag的掺入对Tc影响不大,Tp逐渐升高.由于钙钛矿颗粒属性的改善和金属导电通道的出现,材料的电阻率明显下降.Ag掺杂使室温磁电阻得到显著增强,室温下从x=0.30样品中得到最大的磁电阻,约为32%,是La0.67Sr0.33MnO3样品的8倍,La0.67Sr0.33Mn0.93Ti0.07O3样品的1.6倍.     

Microwave assisted hydrothermal synthesis and magnetocaloric properties of La0.67Sr0.33MnO3 manganite

We report microwave assisted hydrothermal synthesis and magnetocaloric properties of La0.67Sr0.33MnO3 manganite. The synthesized La0.67Sr0.33MnO3 nanoparticles was characterized using X-ray diffraction (XRD), field emission scanning electron microscopy (FE-SEM), energy dispersive X-ray spectroscopy (EDS) and magnetization measurements. The XRD results indicated that La0.67Sr0.33MnO3 nanoparticles have polycrystalline nature with monoclinic structure. FE-SEM results suggested that La0.67Sr0.33MnO3 nanoparticles are assembled into rod like morphology. Magnetization measurements show that La0.67Sr0.33MnO3 nanoparticles exhibit transition temperature (Tc) above room temperature. The maximum magnetic entropy change (deltaS(M))max was found to be 0.52 J/kg K near Tc approximately 325 K at applied magnetc field of 20 kOe. This compound may considered as potential material for magnetic refrigeration near room temperature.