电阻法间接测量居里温度

在磁性材料的实际应用中有时需要测量居里温度．采用电阻法测量在升温过程中电阻的变化从而来推算居里温度．结果表明．一般情况下．随着温度的升高电阻是增大的．当温度在居里点附近．电阻或者处于一稳定值或者有明显偏小现象．根据温度对电阻的影响可知居里点就在此范围内．     

利用RL交流电桥测量磁性材料的居里温度

利用RL交流电桥测量了磁性材料的居里温度,并讨论了工作频率和工作电压的变化对测量结果的影响.     

稀磁半导体材料居里温度的极值点

以Zener模型为基础,考虑反铁磁性交换作用对DMS材料居里温度的影响,理论计算得到了居里温度关于掺杂浓度和反铁磁性交换作用的二元函数,对GaAs ∶ TM(Ga,TM)As (TM=Sc,Ti,V,Cr,Mn,Fe,Co,Ni)的居里温度做了详细分析得到:n型半导体居里温度有一个极大值,而p型掺杂是单调的递增。     

铁磁相变和居里温度的一种直接观测方法

铁磁相变和居里温度的一种直接观测方法王魁香，陆国会，邓京川，卢杰（吉林大学物理系长春１３００２２）一、原理在物理学中，经常遇到相变的问题，日常生活里又很少有相变现象的例子，所以人们对相变的理解很抽象．而铁磁物质（铁磁相）在居里（或临界）温度Ｔｃ转变成...     

居里温度演示装置

铁磁性物质被加热达到居里温度时,会发生由铁磁性向顺磁性转变,这是铁磁性物质的重要特性之一.利用这一特性制造的温控开关已有着广泛的应用,家用电饭煲里的温控开关就是成功的例子之一.大学物理课程中,教师讲授该内容时,由于缺乏相应的演示仪器而难以达到预期的教学效果.以下介绍的演示装置可生动地演示这一物理现象,以弥补这方面的不足.     

不同方法测铁电材料的居里温度

1铁电材料的居里温度及其特性 铁电材料的一些性质总是随温度的变化而变化,而且都有一个临界温度Tc,当超过临界温度时,晶体的分子结构发生变化,自发极化消失,没有铁电性,我们称这个点为居里点,这个温度为居里温度．     

La(Fe,Si)_(13)化合物的居里温度机制

NaZn13型La(Fe,Si)13化合物随Si含量增加,相变性质由一级过渡为二级,化合物晶胞体积收缩,饱和磁化强度降低,居里温度升高.其居里温度与晶胞体积之间的关系不能用Bethe-Slater曲线给出合理的解释.本文利用添加间隙原子碳调节La(Fe,Si)13化合物晶胞体积和居里温度的方法,系统研究了该化合物居里温度与晶胞体积之间的关系.结果发现二者之间的变化规律遵循Jaccarino-Walker模型,即仅有5%甚至更少的3d电子被认为是真正的巡游电子,其余的3d电子仍是局域的.以极化的巡游电子为媒介,局域电子之间产生类似于Ruderman-Kittel-Kasuya-Yosida的长程相互作用,相互作用的符号和大小与距离呈周期性震荡.随Si含量的增加,La(Fe,Si)13化合物巡游电子数目增加,化合物的居里温度由晶胞体积和巡游电子的浓度共同决定.     

活塞圆筒容器中铁磁居里温度的一种测量方法

 本文介绍了在活塞-圆筒型装置中建立的高压下原位测量居里温度的方法。采用简单的测量电路，不需要锁相放大器等精密仪器，系统仍具有较高的灵敏度，足以满足测量小样品的要求。合理的高压组装结构保证了测量的成功率。实验结果表明，测量的重复性误差小于±1 ℃。     

发现MM＇X合金居里温度窗口的启示

人们习惯把具有马氏体相变的合金称为形状记忆合金．20世纪发现的所有形状记忆合金基本没有磁性．     

Chemical and structural disorder effects on the Curie temperature

The disorder effects on the Curie temperature of ferromagnetic and ferroelectric systems are studied by factorizing the spin–spin (or dipole–dipole) interaction into a chemical (on-site) and a structural (off-site) part. Assuming the statistical independence of the two contributions, the Curie temperature T_c is calculated in the limit of small disorder and in the mean-field approximation. The chemical disorder always enhances T_c . In the absence of spin waves (Ising-like systems), the structural disorder enhances T_c in turn. The only negative contribution to T_c is found in Heisenberg-like systems, and is ascribed to the interplay between structural disorder and spin waves. A comparison is made with other mean-field theories that adopt a different representation of the disorder. The application of the results obtained to real systems is considered, with special reference to recent experimental data on ferroelectric perovskites. An approximate expression, consistent with the mean-field approach, is suggested to estimate the relative weight of the chemical and structural disorder effects, even when an exact factorization is impossible, as is the case of the exchange interactions.     

Curie temperature and frustrated phase separation in manganites

There is an increasing experimental evidence that phase separation between insulating and metallic phase plays an important role in the physics of manganites. On general grounds one can argue that the electronic density in the metallic and insulating region will be generally different. This implies that phase separation of the ordinary “Maxwell construction” type is frustrated by the long-range Coulomb interaction. We present a generalization of Maxwell construction to this situation. The system is assumed to separate in islands of one phases hosted by the other. The size of the islands is determined minimizing a free energy that takes into account both surface energy and Coulomb effects. We discuss the peculiarities of this kind of phase separation and the consequences for the manganites. In particular, we present an explanation for the non-monotonous behavior of the Curie temperature as a function of doping.     

Dependence of the Curie temperature on the effective de Gennes factor in ferromagnets with exchange frustration

Considering the magneto-diluted gadolinium-containing Adamian alloys, it is shown that the dependence of the Curie temperature on the de Gennes factor ξ = c(g ? 1)2J(J + 1) can be expanded for ferromagnets with the exchange frustration. It is shown that in this case it is necessary to replace J by S _eff and that the linear dependence of T _C on ξ_eff remains up to the pure spin-glass state with S _eff = 0.     

The role of demagnetization factor in determining the ‘true’ value of the Curie temperature

The Curie temperature, T_C, is the temperature above which a material loses its long-range ferromagnetic order. Considering the equation of state of a ferromagnet in the mean-field approximation it has been shown theoretically that the value of the demagnetization factor N has a significant influence on the perceived location of T_C on the temperature scale. A series of precise measurements of magnetization using two differently shaped single crystals of high-purity gadolinium was carried out to prove this result experimentally and develop a procedure leading to the ‘true’ value of T_C.     

Residual stress and Curie temperature of Fe-N thin films prepared by dc magnetron sputtering at elevated temperature

Fe-N thin films were prepared by dc magnetron sputtering at elevated temperature of 80 °C. The residual stress of the thin film was characterized by means of grazing incidence X-ray diffraction method. The effect of magnetron sputtering parameter on residual stress was investigated. The results indicate that the nitrogen content in working gas has great effects on the residual stress in the Fe-N thin film, and the residual stress increases firstly and then decreases with the increasing of nitrogen content in working gas. Curie temperature measurement shows that tensile residual stress enhances the ferromagnetic-paramagnetic transition temperature of Fe-N thin films under the condition of same phase composition.     

Structure and Curie temperature of Y2Fe17-xCrx

The structures of Y2Fe17-xCrx are simulated by the ab initio potentials. The site preference of Cr atom in Y2Fe17 is evaluated and the order is determined as 4f, 12j, which is close to the experimental result. Based on the site preference behavior, the calculated parameters and the atom sites of Y-Fe-Cr system are studied. The result corresponds well to observed data. Further, the DOS of the relaxed structures are calculated and the variation in Curie temperature is explained qualitatively by the spin-fluctuation theory.     

Electric field dependence of the Curie temperature and microwave absorption in displacive ferroelectrics with impurities II

Expressions for the complex dielectric constant, microwave absorption and the Curie temperature in doped displacive ferroelectrics, subjected to an external electric field are discussed, using the approach made in our previous study. A cross-term of defect parameters with electric field and anharmonic parameters is obtained. The intrinsic parametersB andC are modified by impurity terms. The qualitativeE ² dependence of tan δ is discussed.     

Investigation of magnetic properties of Al substituted nickel ferrite nanopowders, synthesized by the sol-gel method

NiFe_2−xAl_xO₄ nanopowders, where x is from 0 to 1.5 with a step of 0.5, have been synthesized by the sol-gel method and the effect of non-magnetic aluminum content on their structural and magnetic properties were investigated. The X-ray diffraction (XRD) patterns revealed that the synthesized nanopowders are single phase with a spinel structure. Mean crystallite sizes of the samples were calculated by Scherrer's formula and were in the range 20-31 nm. The morphology of the nanopowders was investigated by TEM and the mean particle sizes of the samples were in the range 55-80 nm. Magnetic hysteresis loops were recorded at room temperature in a maximum applied field of 3000 Oe. The results show that by increasing the aluminum content, the magnetizations of the nanopowders are decreased. This reduction is caused by non-magnetic Al³⁺ ions, which by their substitutions the super exchange interactions between different sites will be reduced. It is also seen that the magnetizations of the nanopowders are lower than those related to their bulk counterparts. This reduction was found to be as a consequence of surface spin disorder. M-T curves of the samples were obtained using a Faraday balance and by which the Curie temperatures of the powders were determined. The results that are obtained show that the Curie temperatures of the nanopowders are higher than those of their bulk counterparts.