磁化等离子体的纵向电阻率

从动力论方程出发,推导并讨论了磁化与非磁化等离子体的纵向电阻率。结果是:(1)各向同性磁化等离子体的电阻率约为非磁化者的1.5倍;(2)对各向异性的等离子体而言,磁化后的电阻率约与T_e⊥T_e‖^-5/2成正比,但非磁化时的电阻率则与T_e⊥^-1T_e‖^-1/2成正比。以上的差异主要是来自外磁场对电子运动轨迹的作用。同时本文亦论述了在讨论经典电阻率时,静态屏蔽作用是主要的,而动力屏蔽对电阻率的影响是可以忽略不计的。 关键词：     

Sm2(TM)17合金的磁性(自旋再取向相变)研究

本文研究了Sm₂(FeNiCoM)₁₇合金(M为非磁性组元)的磁性。样品由六角结构无序型的2∶17主相及少量FeNi合金杂相组成。在六角结构的e轴方向(易磁化方向)观察到下述异常现象:低温(273K以下)时的磁化及反磁化曲线发生明显的跃变,跃变时相应的磁场H_r随温度下降而增大;磁滞迴线是蜂腰型的,温度愈低蜂腰愈明显;升温时磁化强度随温度变化(1.5K至居里点T_C)的曲线上出现极大值,其相应的温度T_t随磁场增大而降低;降温时观察到了热磁滞后现象。但在基面(难磁化方向)上及Co含量增多(>18at％)时,样品却表现了正常的铁磁行为。本文提出用磁矩非共线结构排列的自旋再取向相变来解释上述异常现象,并给出自旋倒向所需越过的能垒高度U=9.2×10^-15erg,用设想磁结构的模型得到的磁化强度的计算值与实验值也符合得较好。 关键词：     

CaSO4·(1/2) H2O粉末中结晶水与吸附水1H的Goldman-Shen实验

本文利用Goldman-Shen脉冲序列测量了CaSO₄·(1/2) H₂O样品中结晶水与吸附水¹H的交叉弛豫时间为55.1ms。在实验中,发现剩余窄线的磁化矢量随时间的衰减有三个过程。本文对此现象作了一些分析讨论。     

多层伊辛膜的磁学性质

用变分累积展开(VCE)方法的一阶近似计算了包括最近邻和次近邻作用的多层伊辛膜的磁学 性质,导出了自发磁化强度、矫顽力、居里点、奈尔点、顺磁磁化率及分子场系数与层数的关系表达式,并做了数值计算和讨论. 关键词： 多层膜 伊辛模型 磁化     

取向Pr2Fe14B与Nd2Fe14B多晶磁化曲线的 计算

基于单离子晶场模型,提出了计算稀土-Fe(Co)金属间化合物取向多晶样品磁化曲线的方法.用此方法计算了取向Pr₂Fe₁₄B和Nd₂Fe₁₄ B多晶的高场磁化曲线,计算中使用了拟合化合物单晶磁化曲线得到的交换场与晶场参数.计 算曲线与实验曲线相符合. 关键词： 磁化曲线 晶场 2Fe₁₄B')" href="#">R₂Fe₁₄B     

Nd2(Fe1-xMnx)14B的低温内禀矫顽力

当x<0.5时,Nd₂(Fe_1-xMn_x)₁₄B可形成四方晶体结构,空间群为P4₂/mnm。在低温下,该赝三元化合物的大块铸态样品具有高矫顽力。此矫顽力不依赖于热处理等工艺过程,因此具有内禀性质。内禀矫顽力 _iH_c与样品的成分有关。Nd₂(Fe_1-xMn_x)₁₄B的起始磁化曲线具有传播场H_p,并且H_p的数值与 _iH_c接近。这表明内禀矫顽力是由畴壁钉扎造成的。研究了 _iH_c与温度的变化关系,并估算了钉扎位垒的强度。测量了Nd₂(Fe_1-xMn_x)₁₄B的居里温度和饱和磁化强度。在此赝三元化合物中,交换作用随Mn对Fe的替换而急剧降低。这使得畴壁厚度变窄。Nd₂(Fe_1-xMn_x)₁₄B的磁化和反磁化行为可用窄畴壁的特征来解释。 关键词：     

Bi0.8Pb0.2SrCaCuOy超导体中磁通运动引起的内耗峰

在线性增加磁场的条件下,用变频倒扭摆测量了配比成份为(Bi_0.8Pb_0.2)SrCaCu₂O_y的试样在超导态时磁化过程中的低频内耗。测量温度为95K,试样处于零电阻状态,所用频率为0.5-5Hz.在内耗-场强H曲线上观测到内耗峰,它有如下特点:1)峰高随加场速率H的增大而增大,但随测量频率的增大而降低;2)峰值处的场强为4-6mT;3)当H由非零值突然改变至零时,磁化过程特征内耗消失;4)试样处于正常态时,上述特征内耗消失。认为超导体在磁化过程中的上述特征内耗是量子磁通的运动所引起来的。 关键词：     

"荧光-1"实验装置物理设计

本文主要介绍"荧光-1"实验装置物理参数设计, 并依据半经验公式预估在实验装置上可能达到的磁化等离子体状态参数. 理论设计结果表明: "荧光-1"实验装置最大放电电流1.5 MA, 四分之一周期3 μs, 最大反向磁场4 T; 以此为实验平台, 当θ箍缩线圈内充气压力50 mTorr(D₂气体)时, 形成的等离子体靶直径约为2 cm, 长度17 cm; 等离子体靶密度6.6×10¹⁶ cm^-3, 温度 (T_i+T_e) 约300 eV; 等离子体平均β值为0.95. 该状态参数接近磁化靶聚变所要求的等离子体靶初始状态参数. 关键词： 脉冲功率技术 反场构形 磁化等离子体 磁化靶聚变     

静电场作用下α一LiIO3单晶中子衍射增强现象的理论解释

本文根据(1)在偏振锥光下,用显微镜观察到α-LiIO₃单晶中层状缺陷在静电场作用下的变化;(2)静电场对a-LiIO₃单晶的X射线形貌象的影响;(3)用X射线双晶衍射测得α-LiIO₃单晶晶格参数的不均匀性,指出α-LiIO₃单晶在静电场作用下中子衍射增强现象是由于晶体中的空间电荷(载流子、杂质离子和空位)在宏观尺度缺陷处富集,造成晶格参数有一定梯度。我们对通常计算中子布喇格散射截面的玻恩近似,引入消光修正,得到畸变晶格中子衍射强度公式,可以解释文献[4—6]中观察到的各种现象。 关键词：     

等离子体中四光子的相干散射

本文应用动力学方法计算了均匀非磁化等离子体的电子二级非线性密度涨落,得到了三波在等离子体中相互作用的三级非线性极化率X⁽³⁾和第四波K₄=K₁-K₂+K₃,ω₄=ω₁-ω₂+ω₃的散射功率,与通常的非相干汤姆逊散射相比,其散射信号要大得多,因此,相干四光子散射可以作为等离子体诊断技术的一个重要方法,本文还指出,文献[4]的结果是本文计算的一个简单情况。 关键词：     

The local magnetization of an incomplete ferromagnet

The local magnetization in the vicinity of a nonmagnetic impurity in a Heisenberg ferromagnet is calculated for different temperatures below the Curie point. In the low-temperature region the spin-wave approximation is used and calculations are carried out up to first-order perturbation theory. The deviation of the magnetization from the value in a perfect magnet turns out to be proportional to T^5/2 for very low temperatures. In the region 0.40 T_CC numerical solutions are obtained for a molecular field model, under the assumption that the influence of the impurity has a finite range. Extrapolations of both sets of results fit reasonably well together for the nearest and next nearest neighbours of the impurity.     

Field dependence of magnetic entropy change: Whence comes an intercept?

The magnetic field-induced entropy change in a ferromagnet undergoing a second-order phase transition at the Curie point is maximum near that point. The maximum magnetic entropy change, (-ΔS)_max, is demonstrated to contain, besides the usual term in H^2/3, a small negative term independent of H. Spatial inhomogeneity of real ferromagnetic materials is shown to be the origin of the off-set term, whose magnitude proves proportional to the width of the distribution of local Curie points.     

Experimental determination of the spin-wave spectrum of the two-dimensional ferromagnet K2CuF4

K₂CuF₄ is a quasi-bidimensional ferromagnet with an easy magnetization plane. The Curie temperature is 6.25 K. We have measured the spin-wave spectrum from 2 to 14 K, and found an exchange integral of 11.4 K between the first neighbours in the basal plane. No measurable dispersion was found along the axis perpendicular to that plane. We have observed a shift in the energy of the magnons, and a broadening of the magnon peak both of which behave differently below and above the Curie temperature.     

Critical behavior of La<Subscript>0.825</Subscript>Sr<Subscript>0.175</Subscript>MnO<Subscript>2.912</Subscript> anion-deficient manganite in the magnetic phase transition region

For La _0.825 ³⁺ Sr _0.175 ² +Mn³⁺O _2.912 ^2? anion-deficient manganite, the specific magnetization, the dynamic magnetic susceptibility, and the heat capacity are investigated. This material is found to be an inhomogeneous ferromagnet below the Curie point T _C ≈ 122 K, which is much lower than the Curie point determined for the stoichiometric composition (T _C ≈ 268 K). An increase in magnetic field by two orders of magnitude leads to an increase in the Curie temperature by ΔT ≈ 12 K. The presence of oxygen vacancies leads to the frustration of a part, namely, V _fr ≈ 22%, of the indirect Mn³⁺-O-Mn³⁺ exchange interactions, but the spin glass state is not realized. The ferromagnetic matrix of the material under study is characterized by a scatter in the exchange interaction intensities. The heat capacity is found to exhibit an anomalous behavior. Based on the Banerjee magnetic criterion, it is established that the ferromagnet-paramagnet transition observed for La _0.825 ³⁺ Sr _0.175 ²⁺ Mn³⁺O _2.912 ^2? anion-deficient manganite is a second-order thermodynamic phase transition. The mechanism and origin of the critical behavior of the system under investigation are discussed.     

MuSR study of weakly magnetic Y(Co1−x Al x )2

All previous experiments have suggested that Y(Co_1−x Al _x )₂ is a weak itinerant ferromagnet for 0.12<x<0.20. The muon transverse damping rate (λ) increases rapidly near the Curie point forx≥0.155 and for one sample withx=0.145. The value of λ increases with decreasing temperature for other samples withx<0.155 but shows no feature at the Curie point.     

多基点同伦群理论

本文建立了一个定理:当拓扑空间V单连通时,N(≥1)基点n阶同伦类集合π_n(V;v₁,v₂,…,v_N)可被构造成同构于单基点n阶同伦群π_n(V)的群,叫做N基点n阶同伦群;并且V的单连通性一般是不可省略的条件。给出了一些推论。简要地触及了这个定理及其推论在铁磁状态拓扑分类中的应用问题。 关键词：     

On the mixed valence of the chromium ions in the noncollinear ferrimagnetic spinels Mn1−xCuxCr2S4 (Where x = 0.85, 0.90, 0.95)

For the polycrystalline samples of Mn_1?xCu_xCr₂S₄ (x = 0.85, 0.90, 0.95) the magnetization was measured in the temperature range between 77 K and the Curie temperature, T_C, using a magnetic balance (Faraday's method) and pulsed magnetic fields up to 2.0 T. The magnetic susceptibility was measured between T_C and about 600 K. The Curie temperatures were obtained using the kink point method.In the temperature range between 4.2 and 77 K the magnetization was measured in stationary magnetic fields up to 14 T. The data indicate a noncollinear ferrimagnetic structure. The compounds under investigation can be treated as CuCr₂S₄ slightly doped with Mn, with a valence distribution Mn²⁺_1?xCu¹⁺_xCr³⁺_2?xCr⁴⁺_xS^2?₄.     

Pressure dependence of the weak itinerant ferromagnetism of Y(Co1-xAlx)2

Abstract

Y(Co_1-xAl_x)₂ is a weak itinerant ferromagnet for 0.12 < x < 0.20 with a maximum Curie point of about 25 K near x = 0.15. The pressure dependence of the Curie point for samples with 0.14 < x < 0.18 was measured in the temperature and pressure range 5–25 K and 0–8 kbar using a liquid filled lock cell. It was found that T_c was linear in pressure and extrapolated to OK at P_c = 9 ± 1 kbar for all samples. The volume expansion from YCo₂ to x = 0.15 is equivalent to a chemical pressure of -40 kbar so ferromagnetism cannot occur at the lattice constant of YCo₂.     

The kinetics of relaxation of magnetization fluctuations near the phase transition from paramagnetic state to ferromagnetic state with domain structure

The equations of motion describing relaxation of magnetization fluctuations in the paramagnetic state for a uniaxial ferromagnet have been solved. In the Landau-Ginzburg functional the demagnetization energy has been taken into account. The finite dimensions of a sample have been considered. It has been shown, that a phase transition is generated by fluctuations containing information about the period of the domain structure at the phase transition point T_c¹. The obtained formulae describe T_c¹ and the period of the domain structure. The results can be used both for bulk materials and thin films.     

Deviation from Kittel's magnetic resonance formula near Tc of CdCr2Se4

Approaching the Curie temperature of the cubic ferromagnet CdCr₂Se₄ from above, the g-factor increasingly shifts from the value predicted by Kittel's formula. In the exchange critical region (susceptibility χ ?1) the g-shift is consistent with δg/g ≈ χ² following from the complex self-energy.