多晶La-Pb-Mn-O体材料的巨磁电阻效应

利用固相反应法制备了多晶立方结构的Ｌａ－Ｐｂ－Ｍｎ－Ｏ体材料,材料的铁磁相变温度ＴＣ为２５７Ｋ,其金属－半导体转变温度ＴＰ为２５１Ｋ,外加磁场分别为５Ｔ和１３Ｔ时,材料的巨磁电阻（ＧＭＲ）峰值分别达到了７２％和８５％,在７７Ｋ￣室温的温度范围内,材料都具有ＧＭＲ效应,ＴＰ附近具有ＧＭＲ峰值效应,ＧＭＲ效应与自旋极化行为有关,而ＴＰ附近的ＧＭＲ峰值效应除了与自旋极化子行为有关外,与磁场作用下勒流子自     

La0.67Ca0.33Mno3—δ体材料的巨磁电阻特性

利用高温烧结法制备了多晶立方结构的Ｌａ０．６７Ｃａ０．３３ＭｎＯ３－δ体材料。材料的居里温度（Ｔｃ）为２８０Ｋ，其金属－半导体转变温度（Ｔｐ）为２７０Ｋ，接近于Ｔｃ。外加磁场下的磁电阻（ＭＲ）峰值温度与Ｔｐ十分接近。外加磁场为０．６Ｔ和５Ｔ时，材料的ＭＲ峰置分别过到４０％和７６％，材料具有显著的巨磁电阻效应，在液氮温度附近，也观察到了相当大的磁电阻效应。     

含聚苯胺粒子的电流变液及其性能

研究了分散介质、电场种类、表面活性剂以及工作温度和时间对含聚苯胺（ＰＡｎ）粒子的电流变（ＥＲ）液性能的影响。研究发现，以氯化石腊为分散介质的ＰＡｎ的ＥＲ液的屈服应力（τｓ）最大；ＥＲ液在直流电场比在有效值相同的交流电场作用下产生的τｓ大，电流密度（ｉ）小；随表面活性剂用量的增加，ＥＲ液的τｓ出现最大值，而ｉ和零场屈服应力单调降低。结果表明，无水的ＰＡｎ的ＥＲ液具有高的ＥＲ活性、宽的工作温度区间、低     

环十二酮肟在硫酸中热效应

使用ＲＤ－１型热导式自动量热计测量了不同温度下环十二酮肟在９８％硫酸中热效应。结果表明：当Ｔ＜３３３Ｋ时，仅产生溶解热效应，３０３Ｋ下溶解热△Ｈ＿（ｓ，ｍ）＝－５１．７ｋＪ·ｍｏｌ￣（－１）（ｍ＝４．２８５ｍｏｌ·ｋｇ￣（－１））；当Ｔ＞３４３Ｋ时发生环十二酮肟重排反应，３９３Ｋ下反应热△Ｈ＿（Ｒ，ｍ）＝－２３１．８ｋＪ·ｍｏｌ￣（－１）（ｍ＝４．９６×１０￣（－３）ｍｏｌ·ｋｇ￣（－１））和△Ｈ＿（Ｒ，ｍ）＝－２３７．０ｋＪ·ｍｏｌ￣（－１）（ｍ＝１．７×１０￣（－２）ｍｏｌ·ｋｇ￣（－１））。     

热化学气相反应法制备SiC纳米粉的研究

利用ＳｉＨ４－Ｃ２Ｈ４－Ｈ２系统的反应，在１４２３Ｋ￣１６７３Ｋ温度范围内对ＳｉＣ超细粉的合成进行了系统研究。采用的粉末表征方法有透射电镜（ＴＥＭ）、红外吸收谱（ＩＲ）、Ｘ射线衍射（ＸＲＤ）、粉末比表面分析（ＢＥＴ），高分辨透射电镜（ＨＲＥＭ）和化学分析。结果表明，改变反应温度和反应气体组成比能获得高纯ＳｉＣ超细粉。在１４２３Ｋ￣１５７３Ｋ范围内，粉末富硅，当温度超过１６２３Ｋ时粉末富碳，在Ｔ＝１     

赋值格为非线性序的一种6值逻辑系统K6^1

研究赋值格为非线性序，其格结构不同于Ｂｏｏｌｅ代数，而蕴函算子→取Ｋｌｅｅｎ－Ｄｉｅｎｅｓ算子ＲＫＤ的一种新的６值逻辑系统Ｋ６＾１的语义理论，得到若干结果，特别是Ｋ６＾１中的准重言式恰与Ｃ２中的重言式一致：ＱＴ（Ｋ６＾１）＝Ｔ（Ｃ２）。     

气态膜过程中的热效应

实验表明提高温度（Ｔ）能大幅度增加挥发性物质在气态膜过程中的传质系数（Ｋ），Ｋ和Ｔ间的关系符合Ａｒｒｈｅｎｉｕｓ方程Ｋ＝Ｋｏｅｘｐ（－Ｅ／ＲＴ）。用Ｓｔｏｋｅｓ－Ｅｉｎｔｅｉｎｓ和Ｌｅｖｅｑｅ方程，从理论上证实：（１）对于易挥发性物质（如ＨＣＮ），温度主要是通过降低进水边界层中水溶液的粘度或提高扩散系数，而使传质系数大幅度升高；（２）对于挥发性较小的物质（如苯酚），温度主要是通过提高其蒸汽压或进水     

陶瓷材料高温断裂韧性评价

采用四点弯曲实验方法，研究了高温下不同测试方法（ＣＮ法、ＳＥＮＢ法和ＳＥＰＢ法）对工业用重结晶ＳｉＣ陶瓷材料断裂韧性的影响。通过实验发现：在低温下（Ｔ〈８００℃）不同测试方法所获得的ＫＩＣ不同，ＣＮ法测得ＫＩＣ偏大，而ＳＥＰＢ法测得的ＫＩＣ则偏小，同时，三种测试方法获得的ＫＩＣ随温度的升高变化率都不明显。在高温下（Ｔ〉８００℃），不同的测试方法其ＫＩＣ随温度的和蔼同变化趋势不同，ＣＮ法ＫＩＣ随温度的升高而增大，ＳＥＮＢ法ＫＩＣ随温度的升高而减小，ＳＥＰＢ法ＫＩＣ随温度的升高则基本无变化。     

首架凯能（Kinon）带遥控35mm全自动迷你相机的使用

首架凯能（Ｋｉｎｏｎ）带遥控３５ｍｍ全自动迷你相机的使用杭州叶心德凯能（Ｋｉｎｏｎ）相机，台湾群昌公司（ＦＡＲ－ＳＨＡＲＰ）产品．内地有译作“柯尼”相机的。群昌公司在生产日本元件组装的Ｓｎａｐｓｈｏｔ３０型３５ｍｍ迷你相机基础上，经改进开发出了凯能（...     

乙炔端基砜对聚醚醚酮转变温度的影响

用ＴＢＡ、ＤＳＣ、ＷＡＸＳ研究了乙炔端基砜（ＡＴＳ）对聚醚醚酮（ＰＥＥＫ）的玻璃化温度（Ｔｓ）、冷结晶温度（Ｔｃｃ）、降温结晶温度（Ｔｃ）、熔点（Ｔｍ）和结晶度（Ｘｃ）的影响。ＡＴＳ的加入使ＰＥＥＫ的Ｔｇ、Ｔｃｃ提高，Ｔｃ、Ｔｍ和Ｘｃ降低；退火结晶温度提高，ＰＥＥＫ的Ｔｍ提高，但共混物中ＰＥＥＫ的Ｔｍ和Ｘｃ降低。ＷＡＸＳ结果表明，多步退火结晶可形成两种结晶。     

Nb NMR and Fe EPR study of local magnetic properties of magnetoelectric Pb(Fe1/2Nb1/2)O3

The ⁹³Nb NMR and Fe³⁺ EPR spectra of a magnetoelectric Pb(Fe_1/2Nb_1/2)O₃ (PFN) single crystal as well as of PFN ceramics and nanopowder have been measured. The relation between the chemical disorder and the local magnetic structure has been determined. The data show the occurrence of an antiferromagnetic (AFM) phase transition at 145 and 135 K in both single crystal and ceramic samples, respectively. The AFM phase transition is however essentially smeared out in the nanopowder. Two different Nb sites exist which have different local magnetic fields which are essentialy distributed in value. These two Nb sites correspond to different types of “chemical” order: Fe rich, Nb poor and Fe poor, Nb rich regions. The temperature dependences of the sublattice magnetizations and the values of the superhyperfine fields at the Nb ions are obtained. NMR data suggest that a spin-glass like state of PFN below T = 20 K arises from the Fe poor, Nb rich regions.     

多铁性BaTiO3/La2/3Sr1/3MnO3复合薄膜的制备及其强磁电效应的研究

使用脉冲激光沉积技术,在(001)取向的LaAlO3(LAO)单晶基片上外延生长了BaTiO3/La2/3Sr1/3MnO3(BTO/LSMO)双层复合薄膜.电学和磁学性能的研究显示复合薄膜具有较低的相对介电常数(εr=263),优良的铁电和铁磁性能以及高于室温的铁磁居里温度(Tc=317 K).复合薄膜的磁电电压系数(αE)为176 mV/A,高于同类结构磁电系统一个数量级,相应的界面耦合系数k值为0.68,表明铁磁层和铁电层界面之间存在较大程度的耦合.     

High Field and Low Temperature Magnetization of ErCu2Si2 Single Crystal

The magnetic measurements have been performed for high fields up to 18 T and low temperatures down to 0.5 K on the single crystal compound ErCu₂Si₂. In the temperature dependence of magnetic susceptibility, two anomalies are seen at T _N =1.51 K and T _t =0.97 K which is corresponding to an antiferromagnetic ordering temperature and may come from a change of magnetic structure. Low temperature magnetization shows a metamagnetic transition around 0.4 T along the easy magnetization direction of [001]. The magnetization is almost saturated above 3 T and reaches 8.8μ _B /f.u. at 18 T. A metamagnetic transition appears around 0.5 T in the basal plane magnetization processes as well. The anisotropy within the basal plane is fairly large for high fields. These behaviors have been explained from crystalline electric field effects and magnetic interaction in terms of molecular field.     

Pb(Mn1/3Sb2/3)0.05Zr0.47Ti0.48O3压电陶瓷的温度稳定性研究

探讨了硬性添加物MnO2、软性添加物Nb2O5和两性添加物Cr2O3对锑锰锆钛酸铅Pb(Mn1/3Sb2/3)0.05Zr0.47Ti0.48O3(简称PMSZT5)压电陶瓷的相组成及温度稳定性的影响.研究结果发现:各掺杂组成在900℃的煅烧温度下,都可以得到钙钛矿结构.随着各掺杂离子的增大,四方相含量减少,准同型相界向三方相移动.综合考虑离子掺杂对PMSZT5压电陶瓷的机电性能及温度稳定性的研究结果表明:锰过量较其它铌和铬掺杂的温度稳定性更好,机电性能最佳的PMSZT5+0.1wt%MnO2的组成,ε33T/ε0=1560,d33=350pC/N,Kp=0.63,25~80℃的fr、K31和d31平均温度系数分别为72×10-6/℃、0.027%/℃和0.100%/℃.     

Influence of Nb5+ Doping on Structure and Electrochemical Properties of Spinel Li1.02Mn2O4

The Li1.02NbxMn2-xO4 (x=0,0.005,0.01,0.02,0.04 and 0.1) materials were prepared by solid-state reaction method in which Li2CO3 , electrolytic MnO2 and Nb2O5 were used as reactants. The influences of the Nb5+ doping on structure, morphology and electrochemical performance were systemically investigated by means of X-ray diffraction (XRD), scanning electron microscopy (SEM), cyclic voltammetry (CV) and AC impedance. XRD test showed that the prepared samples had single spinel structure although there was impurity phase of LiNbO3 existing in Li1.02NbxMn2-xO4 phase after Nb5+ doping. The doped materials with Nb5+ had smaller lattice parameters and crystal volume compared with pristine Li1.02Mn2O4. The endurance of overcharge was largely improved. In addition, the small amount of Nb5+ doping could increase the material conductivity.     

Complete set of material properties of [011](c) poled 0.24Pb(In(1/2)Nb(1/2))O(3)-0.46Pb(Mg(1/3)Nb(2/3))O(3)-0.30PbTiO(3) single crystal

A complete set of elastic, piezoelectric, and dielectric constants of [011](c) poled multidomain 0.24Pb(In(1/2)Nb(1/2))O(3)-0.46Pb(Mg(1/3)Nb(2/3))O(3)-0.30PbTiO(3) ternary single crystal has been determined using resonance and ultrasonic methods and the temperature dependence of the dielectric permittivity has been measured at 3 different frequencies. The experimental results revealed that this [011](c) poled ternary single crystal has very large transverse piezoelectric coefficient d(32) = -1693 pC/N, transverse dielectric constant ε(11)/ε(0) ~ 7400 and a high electromechanical coupling factor k(32) ~ 90%. In addition, its coercive field is 2 times of that of the corresponding binary 0.7Pb(Mg(1/3)Nb(2/3))O(3)-0.30PbTiO(3) single system with much better temperature stability. Therefore, the crystal is an excellent candidate for transverse mode electromechanical devices.     

Anisotropic and excellent magnetocaloric properties of La0.7Ca0.3MnO3 single crystal with anomalous magnetization

Magnetic properties and the magnetocaloric effect (MCE) have been investigated in La_0.7Ca_0.3MnO₃ single crystal with applied field along both the ab-plane and the c-direction. Due to the magnetocrystalline anisotropy, the crystal exhibits anisotropy in the MCE. Upon application of a 5 T field, the magnetic entropy changes (ΔS_M), reaching values of 7.668 J/(kg K) and 6.412 J/(kg K) for both the ab-plane and the c-direction, respectively. A magnetic entropy change of 3.3 J/(kg K) was achieved for a magnetic field change of 1.5 T at the Curie temperature, T_C = 245 K. Due to the absence of grains in the single crystal, the ΔS_M distribution here is much more uniform than for gadolinium (Gd) and other polycrystalline manganites, which is desirable for an Ericsson-cycle magnetic refrigerator. For a field change of 5 T, the relative cooling power, RCP, reached 358.17 J/kg, while the maximum adiabatic temperature change of 5.33 K and a magnetoresistance (MR) ratio of 507.88% at T_C were observed. We analysed the magnetization of La_0.7Ca_0.3MnO₃ single crystal at T_C and estimated several parameters of spin fluctuation on the basis of a self-consistent renormalization theory of spin fluctuations, with reciprocal susceptibility above T_C. We found that the magnetic property of La_0.7Ca_0.3MnO₃ is weakly itinerant ferromagnetic. A large reversible MCE and no hysteresis loss with a considerable value of refrigerant capacity indicate that La_0.7Ca_0.3MnO₃ single crystal is a potential candidate as a magnetic refrigerant.     

Thermoelectric properties of the n-type 85% Bi2 Te3-15% Bi2 Se3 alloys doped with Sbl3 and CuBr

The temperature dependence of the Hall mobility, Seebeck coefficient, electrical resistivity, thermal conductivity, and figure-of-merit of the SbI3 and CuBr-doped 85% Bi2Te3-15% Bi2Se3 single crystals have been characterized at temperatures ranging from 77 K to 600 K. The scattering parameter in 85% Bi2Te3-15% Bi2Se3 single crystal was determined as 0.1 from the temperature dependence of the carrier mobility. With increasing the amount of Sbl3 or CuBr doping, the Seebeck coefficient of 85% Bi2Te3-15% Bi2Se3 decreased and the temperature at which the Seebeck coefficient shows a maximum shifted to higher temperature. Compared to the Sbl3-doped specimens, the CuBr-doped single crystals exhibited higher (m* / m0)3/2 c, implying that CuBr is a more effective dopant to improve the material factor and thus the figure-of-merit of 85% Bi2Te3-15% Bi2Se3. The maximum figure-of-merit of 2.0 × 10–3/K and 2.2 × 10–3/K was obtained for 0.1 wt % Sbl3-doped specimen and 0.03 wt % CuBr-doped specimen, respectively.     

Effect of Nb substitution on the structural, dielectric and magnetic properties of multiferroic BiFe1−xNbxO3 ceramics

Polycrystalline BiFe_1−xNb_xO₃ ceramics have been synthesized by standard solid-state reaction method. The effect of Nb substitution on the dielectric, magnetic and magnetoelectric properties of the BiFeO₃ multiferroic perovskite was studied. X-ray diffraction pattern revealed that all the samples with x = 0.00-0.10 showed rhombohedral perovskite structure. We obtained single phase upto doping concentration of x = 0.05 and with further increase in Nb concentration, some impurity peaks appeared. An anomaly in the dielectric constant (?) and dielectric loss (tan (δ)) in the vicinity of the antiferromagnetic Néel temperature (T_N) was observed. Nb substitution reduced the antiferromagnetic Néel temperature (T_N) in BiFe_1−xNb_xO₃. Proper amount of Nb could decrease the dielectric loss. Magnetic hysteresis loops measured at 5 K/300 K and temperature dependent magnetization curves indicated ferromagnetism in Nb substituted BiFeO₃ ceramics. The room temperature magnetic moment was found to increase with increase in Nb concentration. The dependence of dielectric constant on the magnetic field is an evidence of magnetoelectric coupling in BiFe_1−xNb_xO₃ ceramics.     

The study of the electric and magnetic properties of PbZr0.2Ti0.8O3-BiFeO3 multilayers

The results of the electric and magnetic measurements performed on PbZr_0.2Ti_0.8O₃-BiFeO₃ symmetric structures, deposited on Pt/Si wafers, were compared for different number of layers in order to analyse the effect of interfaces over the macroscopic properties. It was found that the shape and magnitude of the capacitance-voltage characteristic, as well as the shape and parameters of the ferroelectric and magnetic hysteresis, depend on the number of interfaces in the intended multilayer structure. A temperature induced gradual transition from a magnetically disordered spin glass like phase of low temperature to an uncompensated antiferromagnetic phase at room temperature takes place in the BiFeO₃ films, under low applied magnetic fields. A partial ferromagnetic like order can be obtained at low temperatures by increasing the field. The observed changes in the electric and magnetic behaviour of the systems were related to an increased degree of disorder for electric dipoles and magnetic moments, due to the increased number of layers and crystallization treatments.