Numerical modeling and simulation of temperature distribution uncertainty subject to ferromagnetic thermoseeds hyperthermia

In the process of ferromagnetic thermoseeds mediated magnetic induction hyperthermia, the tempera- ture distribution in the tumor region is a key factor to determine the therapy effect. During the preoperative treatment planning, discrepancies of the treatment parameters may lead to the temperature distribution uncertainty within the target area. Inaccurate prediction of temperature distribution may induce the treatment failure; therefore, it would be significant to investigate the uncertainty of tissue temperature prediction caused by the disturbance of calculation parameters. In this paper, 3D temperature field and necrosis zone of tissues in ferromagnetic thermoseeds hyperthermia are simulated by the finite volume algorithm, and effects of parameter uncertainties on the temperature distribution are revealed. Results show that selecting appropriate magnetic field parameters for treatment is a priority to guarantee therapeutic effect. Thermoseed properties and blood perfusion rate are the obvious disturbing terms for temperature distribution, while the metabolic heat of bio-tissues can often be ignored within limits. Our investigation is of importance for guiding reasonable and optimal preoperative treatment planning.     

铁磁材料的磁路图解法计算

用试探法计算无分支不均匀恒定磁通磁路的反面问题的计算相当繁琐。本文推导找出一种快捷准确求磁通的方法——图解法。     

钙铁硅铁磁体微晶玻璃的制备

在 Fe_2O_3-CaO-SiO_2-B_2O_3-P_2O_5五元系统中制备出能用于温热治疗肿瘤的铁磁体微晶玻璃热种子材料。在1000℃热处理得到的微晶玻璃磁铁矿晶粒尺寸约为70nm,最大比饱和磁化强度为394.6A·m~2/kg。并证实形成玻璃的氧化铁最大含量为37.7%,必须在还原气氛下进行热处理才能得到以磁铁矿为主要晶相的铁磁体微晶玻璃。     

铁磁-反铁磁双层系统低温内能

应用线性自旋波的理论导出铁磁－反铁磁双层系统的Ｈｅｉｓｅｎｂｅｒｇ模型哈密顿量,采用矩阵格林函数运动方程技术得到自旋波的色散关系,利用数值计算的方法得到铁磁－反铁磁双层的低温内能。     

铁磁条对石墨烯中谷依赖电子输运性质的影响

本文建立了铁磁条和硬势垒共同调制下的石墨烯纳米结构模型,计算了铁磁条产生的磁场的大小和铁磁条的宽度对石墨烯中谷依赖的电子输运性质的影响,重点研究了该石墨烯纳米结构中电子的电导和谷极化特征. 数值计算结果表明,该纳米结构中可实现显著的谷极化效应,且磁场的大小和铁磁条的宽度均会对其中的电子电导和谷极化产生较大的影响. 因此,我们可以通过控制铁磁条的宽度和其产生的磁场的大小来获得实际需要的谷极化强度. 这项研究有助于理解和设计谷电子学设备.     

铁磁质斯特林制冷循环的主要特性

给出铁磁质的热力学性质,并由此讨论了磁斯特林制冷循环的性能,得到一些普遍的结论。     

单原子层磁性纳米带的自旋波谱

本文利用量子统计理论的多体格林函数方法计算了单原子层磁性纳米带的自旋波的色散关系。带宽为L的纳米带,其自旋波能谱有L条,自旋波能量随温度的升高而降低。温度接近居里点时,自旋波能量趋于零,可以称之为模式的软化。零温时,准一维纳米带体系的自旋波能量曲线随带宽的变宽而上升,最后趋于二维平面的数值。把单原子层磁性纳米带与单壁磁性纳米管的自旋波能谱做比较,前者的自旋波能量是非简并的,后者是简并的。自旋波能量简并在物理上是由对称性所致,与纳米管相比,纳米带的几何对称性明显降低了。     

Ferromagnetic and ferroelectric properties of Aurivillius phase Bi9Fe4.7Me0.3Ti3O27（Me 5 Fe,Co, Ni,Mn）

New Aurivillius phase Bi9Fe4.7Me0.3Ti3O27（Me = Fe, Co, Ni, Mn） oxides have been prepared using a citrate combustion method. X-ray diffraction on powders and high-resolution transmission electron microscopy investigation confirmed that the Bi9Fe4.7Me0.3Ti3O27 samples are with an eight-layer structure. Both ferromagnetic and ferroelectric investigations suggested that Co or Ni substitution could enhance their multiferroic properties,while Mn substitution depressed them. Among all the samples, Bi9Fe4.7Co0.3Ti3O27 sample exhibits the largest remnant polarization of Pr＊3.8 l C/cm2, and the largest remnant magnetization of Mr＊0.06 lB/f.u. with a Curie temperature about 764 K, while the Bi9Fe4.7Ni0.3Ti3O27 sample has the largest spontaneous magnetization（0.26 lB/f.u.）. The improved ferromagnetic properties ofboth Bi9Fe4.7Co0.3Ti3O27 and Bi9Fe4.7Ni0.3Ti3O27 can be ascribed to the spin canting of magnetic ion-based sublattices via the Dzyaloshinskii–Moriya interaction and also the magnetic ions exchanging interactions（Fe3–O–Co3or Fe3–O–Ni3）.     

双二次耦合场对铁磁/反铁磁双层膜中交换偏置场的影响

研究了界面双线性耦合和双二次耦合对铁磁/反铁磁双层膜中交换偏置场的影响.结果表明:随着双线性耦合场或双二次耦合场的增加,交换偏置场的最大值位置向易轴靠近.另外,交换偏置场随外磁场角度的变化曲线随着双二次耦合场的增加,逐渐趋于正弦图像.其根源在于双二次耦合场与铁磁层单轴各向异场二者作用相互抵消,使曲线趋于光滑.铁磁层的磁滞回线对双二次耦合场也有一定的依赖.     

NM/FS1/FS2/NM结的隧穿电导和隧穿磁电阻

利用平均场近似和转移矩阵方法,对NM/FS1/FS2/NM结(NM为非磁金属,FS1和FS2为铁磁半导体层)的隧穿磁电阻(TMR)与FS层厚度及Rashba自旋轨道耦合的关系进行了研究.结果表明NM/FS1/FS2/NM结中TMR值随半导体层厚度的改变发生周期性变化,选择适当的半导体层的厚度和Rashba自旋轨道耦合系数可以得到大的TMR值.