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1.
李广  姜勇  孙霞  汤萍  黄真  王胜  袁松柳 《物理学报》2000,49(1):124-127
实验上研究了液氦温区La2/3Ca1/3Mn1-xCuxO3(x=0-15)单相多晶样品给定磁场下的电阻随时间的变化,发现磁电阻随时间变化并非遵从对数规律而是呈指数型变化行为.对这一指数型磁电阻弛豫行为的可能起因进行了讨论,指出这是与Mn位上Cu掺杂将额外磁性杂质引入到样品中有关 关键词:  相似文献   

2.
徐明祥  焦正宽 《物理学报》1998,47(6):1006-1011
采用固态反应法制备了In替代的(La2/3Ca1/3)(Mn(3-2x)/3In2x/3)O3(x=0.00,0.10,0.15)体系.通过测量其零场和1.6T磁场下样品的电阻-温度关系以及一定温度下磁电阻率与磁场的关系.发现随In3+替代量的增加其磁电阻峰和电阻峰均向低温方向移动,同时巨磁电阻效应减弱,磁电阻峰也展宽.这是由于In3+替代量的变化,引起 关键词:  相似文献   

3.
 研究了制备压力对纳米块状样品La2/3Sr1/3MnO3的结构、磁学和电学性质的影响。结果表明:样品的晶粒尺寸随制备压力的增加而变小,且不同样品的磁电阻效应不同。低场磁电阻效应在整个实验温区都随制备压力的升高而变弱,这主要是由制备压力使样品晶粒界面连接更紧密所导致;T<200 K时,高场磁电阻效应随制备压力的升高而变强,T>200 K时,高场磁电阻效应随制备压力的升高反而变弱,这主要是由制备压力改变样品的晶粒尺寸所引起。  相似文献   

4.
利用具有多自旋态的Co离子进行Mn位替代,制备了La2/3Ca1/3Mn1-xCoxO3 (0≤x≤0.15) 系列样品并研究了体系的结构和输运特性.结果表明,在替代范围内,样品呈现很好的单相结构,各晶格参数随替代量的增大而减小;Co替代导致体系出现电输运反常,具体表现为在居里温度TC以下电阻-温度曲线的二次金属-绝缘转 关键词: Mn位替代 双峰现象 自旋结构 磁电阻效应  相似文献   

5.
对1/f噪声缺口的超巨磁电阻Pr2/3Sr1/3MnO3薄膜样品从10K到室温的热电势值进行了测量,热电势为负值,低温下随温度线性变化,表现为金属扩散热电势,在150K开始急剧减小,过渡到与温度T成反比的变化关系,与小极化子模型相符.结合在电阻极大温度附近对电阻和1/f噪声行为的讨论,对于发生在电阻极大温度附近的相变过程,结果支持源于相分离的渝渗模型.  相似文献   

6.
对Ce掺杂锰氧化物 (La1 -xCex) 2 3Ca1 3MnO3(x =0— 1.0 )多晶样品的结构和输运性质系统研究的结果 .实验表明 ,在低掺杂浓度下 ,样品呈现完整的正交钙钛矿结构 ;随掺杂浓度的增加 ,有少量CeO2 杂相出现 ,同时伴随有Ce3 和Ce4 离子两种价态的涨落和Mn2 Mn3 Mn4 混合价态的共存 ,Ce掺杂导致的体系无序度增加 ,使得绝缘体 -金属 (I M)和顺磁 -铁磁 (PM FM)转变温度向低温方向移动 .有趣的是 ,Ce掺杂样品的电阻率测量I M转变峰值温度TIM 较PM FM转变温度Tc 为高 ,其差值ΔT(=TIM -Tc)随Ce掺杂含量的增加而增加 ,最大差值ΔT达 5 0K .各样品的磁电阻则随温度的降低而增加 ,在Tc 附近MR达到最大值 ,且随Ce掺杂含量增加Tc 附近的MR最大值迅速增加 ,达到 10 4 %以上 ,表现出很强的庞磁电阻效应 .在x≥ 0 .7时 ,磁电阻效应则表现出反常减小 .整体上而言 ,各样品的磁特性与输运行为间有较强的关联 ,电输运特性可用双交换作用模型进行很好的解释 ,在高温区满足热激活模型 .最后 ,在Ce掺杂对Tc 和MR的影响机理方面进行了初步讨论 .  相似文献   

7.
采用溶胶-凝胶法并经不同温度烧结而制备了名义组分为La2/3Ca1/3MnO3和La2/3Ca1/3Mn1-xCuxO3(x=4%)的系列样品,对它们进行了阻温关系测量.从试验结果观察到:在La2/3Ca1/3MnO3样品中,降温和升温测量的阻温曲线几乎完全重合,没有观察到明显的热弛豫现象.而在不同温度烧结的La2/3Ca1/3Mn1-xCuxO3(x=4%)样品中,阻温关系有明显的热弛豫现象.同时试验还观察到该热弛豫现象随样品烧结温度(颗粒尺寸)的增加逐渐消失.  相似文献   

8.
谈国太  陈正豪 《物理学报》2007,56(3):1702-1706
通过X射线粉末衍射数据,用Rietveld精修方法分析了Te部分替换LaMnO3中La后,其晶格参数及其结构对称性所发生的变化.结果表明:Te掺杂LaMnO3系列样品具有R3C的晶格结构对称性,其MnO6八面体晶格还产生了伸张畸变,畸变程度随Te掺杂量的增加而增大.此外根据Mn—O—Mn键角、eg电子能带的带宽、A位离子平均半径及A位离子尺寸失配度等的变化特点,推测Te掺杂LaMnO3样品除居里温度等相变物理量将随x增加而非线性变化外,还可能产生自旋玻璃态、相分离等宏观现象. 关键词: 庞磁电阻效应 La-Te-Mn-O X射线衍射 Rietveld精修  相似文献   

9.
(La2/3Ca1/3)O3低温下的电阻极小值行为   总被引:3,自引:0,他引:3  
对B位替代的Mn氧化物(La2/3Ca1/3)O3样品在温度远低于居里温度时的电阻率随温度的变化行为进行了研究.发现未加磁场时,样品在低温下表现出电阻率极小行为,这一极小现象在外加磁场后被大为抑制.作者对此实验现象作了定量的理论与实验的比较,并给出了有关可能的机理.  相似文献   

10.
系统研究了强关联锰氧化物La5/8Ca3/8Mn1-xCoxO3(x=0,0.05)体系的结构和输运特性.结果表明,样品均为很好的正交O′单相结构,Mn位5%Co掺杂明显影响了样品铁磁-顺磁(FM-PM)转变和金属-绝缘体(M-I)转变,M-I转变温度TM-I从未掺杂时的271K降至227K,对应的峰值电阻率ρp增大;随着TM-I的降低,Tc同时降低,磁电阻MR%亦相应增加;La5/8Ca3/8MnO3样品在Tc以下表现出长程铁磁有序态,Mn位5%Co掺杂样品则表现为团簇玻璃型短程铁磁有序行为.证明Co掺杂引起电子的局域化效应乃是导致体系输运行为发生变化的主要原因.同时,从Mn3 -O2--Mn4 双交换(DE)作用和超交换(SE)相互作用机制等出发,对样品的输运行为、CMR效应以及与Co掺杂之间的关联进行了讨论.  相似文献   

11.
Replacement of one half of the neodymium ions by lanthanum in Nd2/3Sr1/3MnO3 is shown to result in a considerable increase in the Curie temperature. The single-crystal La1/3Nd1/3Sr1/3MnO3, whose Curie point lies at 315 K, has been found to exhibit a record-high magnetoresistance of 27% in a weak magnetic field of 8.4 kOe in the temperature range above room temperature.  相似文献   

12.
Spherical LiNi1/3Co1/3Mn1/3O2 was successfully prepared by controlled crystallization. The preparation started with the spherical coprecipitate of Ni1/3Co1/3Mn1/3CO3 from NiSO4, CoSO4, MnSO4, NH4HCO3, and NH3·H2O, followed by pyrolysis of Ni1/3Co1/3Mn1/3CO3 at 600°C for 3 h. The X-ray diffraction analysis showed that the homogeneous cubic (Ni1/3Co1/3Mn1/3)3O4 was obtained after the pyrolysis. Spherical LiNi1/3Co1/3Mn1/3O2 was obtained by sintering of the mixture of as-obtained (Ni1/3Co1/3Mn1/3)3O4 and LiOH·H2O at 900°C for 6 h in air. As-prepared spherical LiNi1/3Co1/3Mn1/3O2 presented initial discharge capacity of 162.9 mA h g−1 and capacity retention of 98% at 50th cycle.  相似文献   

13.
Highly crystalline layered Li1?xNaxNi1/3Co1/3Mn1/3O2 (x?=?0, 0.001, 0.01, 0.03, 0.05) materials are synthesized by molten salts method and characterized by scanning electron microscopy, inductively coupled plasma (ICP), X-ray diffraction, Rietveld refinement, and electrochemical measurement, respectively. ICP, SEM, and EDS results show that Na ions are incorporated in LiNi1/3Co1/3Mn1/3O2. Rietveld refinement results show that suitable Na substitution leads to stable layered structure by full Na occupying in Li layer and further attributes to low cation mixing. Electrochemical studies demonstrate that the Na-substituted LiNi1/3Co1/3Mn1/3O2 shows improved rate capability and cycling performance compared to that of pure LiNi1/3Co1/3Mn1/3O2.  相似文献   

14.
Structural, electric and magnetic properties of Ba3Mg1−xCoxNb2O9 based dielectric ceramic compounds have been studied. The samples, prepared by a solid state reaction method, were characterised by X-ray powder diffraction (XRPD), electron microscopy (SEM), dielectric (ε(T)) and magnetic measurements (χ−1(T)). The XRPD analyses showed that the crystal structure of these compounds does change by the increase of substitution degree, passing from a superstructure hexagonal-type, (no. 164), space group (SG) to a simple structure cubic-type, (no. 221), SG. However, the evolution of the elementary unit cell lattice parameter can be followed and it exhibit a linear increasing tendency with increase in the substitution, indicating the existence of a solid solution through out the investigated range of substitution (0-1). The microstructure analysis shows a variation in the grain size and also the porosity of the samples with the degree of substitution. The results are in good agreement with that of dielectric measurements, which also showed that the dielectric constant (ε) increases with the increase of cobalt content. The magnetic characterization of cobalt substituted samples showed an antiferromagnetic type super-exchange interaction between these magnetic ions. At the same time, the values of effective magnetic momentum (μeff) are close to the value that corresponds to Co2+ free ions. The study highlights the possibility of modelling these materials by substitutions, in order to improve properties of negative-positive-zero (NPO) type dielectric applications.  相似文献   

15.
Ceramic samples of (1−x)SrTiO3-xSrMg1/3Nb2/3O3 and (1−x)SrTiO3-xSrSc1/2Ta1/2O3 were prepared, and their dielectric properties were studied at x=0.005–0.15 and 0.01–0.1, respectively, at frequencies 10 Hz–1 MHz and at temperatures 4.2–350 K. A giant dielectric relaxation was observed in the temperature range 150–300 K, and not so strong but well-developed relaxation was found in the temperature range 20–90 K. The activation energy U and the relaxation time τ0 were determined to be 0.21–0.3 eV and from 10−11 to 10−12 s for the high-temperature relaxation and 0.01–0.02 eV and 10−8–10−10 s for the low-temperature relaxation, respectively. The additional local charge compensation of the heterovalent impurities Mg2+ and Nb5+ (or Sc3+ and Ta5+) by free charge carriers or the host ion vacancies is suggested to be the underlying physical mechanism of the relaxation phenomena. On the basis of this mechanism, the Maxwell-Wagner model and the model of reorienting dipole centers Mg2+ (or Sc3+) associated with the oxygen vacancy are proposed to explain the high-temperature relaxation with some arguments in favor of the latter model. The polaron-like model with the Nb5+-Ti3+ center is suggested as the origin of the low-temperature relaxation. The reasons for the absence of ferroelectric phase transitions in the solid solutions under study are also discussed. From Fizika Tverdogo Tela, Vol. 44, No. 11, 2002, pp. 1948–1957. Original English Text Copyright ? 2002 by Lemanov, Sotnikov, Smirnova, Weihnacht. This article was submitted by the authors in English.  相似文献   

16.
The luminescence properties of K(1/2)Bi(1/2)TiO(3):Pr(3+) and Na(1/2)Bi(1/2)TiO(3):Pr(3+) powders are investigated in the temperature range 10-600 K. The experimental data are interpreted on the basis of metal-to-metal charge transfer processes and by considering Bi(3+)-to-Pr(3+) sensitization effects.  相似文献   

17.
ZrO2-coated LiNi1/3Co1/3Mn1/3O2 materials were prepared by hydroxide precipitation. The structure and electrochemical properties of the ZrO2-coated LiNi1/3Co1/3Mn1/3O2 were investigated using X-ray diffraction, scanning electron microscope, and charge–discharge tests, indicating that the lattice structure of LiNi1/3Co1/3Mn1/3O2 were unchanged after the coating but the cycling stability was improved. As the coating amount increased from 0.0 to 0.5 mol.%, the initial capacity of the coated LiNi1/3Co1/3Mn1/3O2 decreased slightly; however, the cycling stability increased remarkably over the cut-off voltages of 2.5~4.3 V and the capacity retention reached 99.5% after 30 cycles at the coating amount of 0.5 mol.%. ZrO2 coating also improved the cycling stability of LiNi1/3Co1/3Mn1/3O2 over wider cut-off voltage of 2.5~4.6 V.  相似文献   

18.
TiO2-coated LiNi1/3Co1/3Mn1/3O2 materials were prepared by the hydrolyzation of Ti(OBu)4. The impact of TiO2 coating on the structure and electrochemical properties of LiNi1/3Co1/3Mn1/3O2 was investigated using X-ray diffraction, scanning electron microscope, and charge–discharge tests. The results indicated that TiO2 coating did not affect the lattice of LiNi1/3Co1/3Mn1/3O2, but exhibited obvious effects on its discharge capacity and cycling stability. As coated TiO2 increased from 0.0 to 2.0 mol%, the initial capacity of samples decreased slightly, but the cycling stability over 2.5∼4.3 V increased remarkably. The capacity retention reached 99.5% at the 50th cycle at a coating amount of 2.0 mol%.  相似文献   

19.
The time dependences of the optical transmission, velocity of sound, and elastic constants at room temperature in a number of the [001]-oriented PbIn1/2Nb1/2O3–PbMg1/3Nb2/3O3–x PbTiO3 single crystals with the compositions lying both far from the morphotropic phase boundary and in its vicinity have been investigated. The analysis of the data obtained has been carried out. It has been shown that, in all the studied crystals, phase transitions induced by an electric field occur in two stages: the first stage is an incubation period associated with a small increase in the polarization of a part of the sample being in the glass phase, and the second phase (after the incubation period τ) is a rapid increase in the polarization and the formation of a long-range order. It has been found that the time τ depends on how close is the temperature of measurements to the Vogel–Fulcher temperature T f . The closer is the temperature of measurements to the Vogel–Fulcher temperature T f , the weaker is the electric field required to be applied to the sample in order to induce a ferroelectric phase. It has been demonstrated that the phase state of the studied crystals is unstable, which manifests itself in a strong dependence of the incubation period τ on the time between the annealing of the sample and the beginning of the measurements. The stability of the phase state depends on the PbTiO3 concentration: an increase in the concentration leads to a significant increase in the stability.  相似文献   

20.
The specific features of the dielectric and pyroelectric responses of a solid solution in the barium-doped multicomponent yPbZn1/3Nb2/3O3-mPbMg1/3Nb2/3O3-nPbNi1/3Nb2/3O3-xPbTiO3 system of the composition y = 0.0982, m = 0.4541, n = 0.1477, and x = 0.3 near the morphotropic phase boundary have been investigated. It has been assumed that the maxima revealed in the dependences of the reversible permittivity on the electric field strength with both the forward and backward changes in the field (E =) are associated with the induced phase transition. Based on the experimental results, the E-T phase diagrams are constructed in the temperature range from ?100 to 150°C for different temperature-field regimes: (i) variation in the electric field E = at a fixed temperature of the sample and (ii) variation in the temperature of the sample at a constant value of E =. It has been found that there is a singular point in the E-T phase diagram and that, in the vicinity of this point, the dielectric and pyroelectric responses of the studied ceramics exhibit specific features.  相似文献   

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