纳米复合永磁Pr9Fe74Co12B5Snx(x=0,0.5)的磁化行为与磁黏滞性

用熔体快淬法制备了纳米复合永磁样品Pr9Fe74Co12B5与Pr9Fe74Co12B5Sn0.5,分析了样品的起始磁化、反磁化过程,测得样品的总磁化率、可逆磁化率以及样品的磁黏滞性.结果表明,两样品在室温下均表现为单一硬磁相磁化行为,在低温下表现为双相行为,且由于添加Sn后使晶粒均匀化从而导致样品低温下的双相行为更加明显.添加Sn后引起样品中软磁相含量和软磁相晶粒尺寸的增加,使磁化反转中可逆磁化部分增多,且使反磁化形核场降低.磁黏滞性研究表明,热激活体积与软磁相晶粒的大小有关.     

非晶态FeZrB合金的电阻率与温度的关系

本文研究了非晶态(Fe_1-xZr_x)_84.5B_15.5(x=0,0.02,0.04,0.06,0.08,0.1,0.15)和Fe_90-xB_xZr₁₀(x=0,4,10,16,20)合金的电阻率ρ与温度T的关系。实验结果表明,当Zr含量在0.02≤x≤0.08时,ρ-T曲线出现两个线性斜率,在略高于居里温度T_c处出现转折,在T关键词：     

非晶态Fe87-xSixB13合金的磁化强度、电阻与温度的关系

本文研究了非晶态Fe_87-xSi_xB₁₃(x=0,9.6,14.5)合金的饱和磁化强度、电阻率与温度的关系。得到样品的居里温度T_C和晶化温度T_cr随Si含量的增加而明显提高。低温下的热磁关系符合布洛赫的T^3/2定律,计算出自旋波劲度系数D从x=0时的62meV·A²增加到x=14.5时的111meV·A²。从D值和Handrich理 关键词：     

非晶态Fe_(87-x)Si_xB_(13)合金的磁化强度、电阻与温度的关系

本文研究了非晶态Fe_(87-x)Si_xB_(13)(x=0,9.6,14.5)合金的饱和磁化强度、电阻率与温度的关系。得到样品的居里温度T_C和晶化温度T_(cr)随Si含量的增加而明显提高。低温下的热磁关系符合布洛赫的T~(3/2)定律,计算出自旋波劲度系数D从x=0时的62meV·A~2增加到x=14.5时的111meV·A~2。从D值和Handrich理论分别推算出表示交换积分涨落的δ=<△J>~(1/2)/值相近。三个样品在低温区都出现电阻率的极小值,电阻率极小值的温度T_(min)从x=0时的10.5K增加到x=14.5时的24.6K。在T_(min)≤T≤130K和室温附近,电阻率分别与T~2和T成线性关系。用推广的Ziman理论讨论样品的电阻率与温度的关系。     

(Tb,Dy)Fe_2金属间化合物的巨大磁致伸缩

一、引言 在铁磁金属和合金中,Ni,Fe-Co,Fe-Ni,Fe-Al等合金都是较好的磁致伸缩材料。它们的纵向饱和磁致伸缩都不过10~(-6)。最常使用的纯Ni的λ_s 仅约—35 ×1O~(-6)。 1971年Clark等报道,稀土-铁Laves相化合物在室温下尚有极大的磁致伸缩值。例如Tb-Fe_2在25KOe下,磁致伸缩高达λ_(11)～1750×10~(-6),约为Ni的五十倍。这类材料可能在高功率换能器及声路器件方面有重要应用。     

(Tb,Dy)Fe2金属间化合物的巨大磁致伸缩

关键词：     

非晶态Fe_(13.3)Ni_(69.6)B_(16.2)Si_(0.9)的结构驰豫

本文讨论了非晶合金Fe_(13.3)Ni_(69.6)B_(16.2)Si_(0.9)的结构弛豫动力学及可逆弛豫过程,研究了各种热处理引起居里温度T_C的变化。发现经长时间退火后T_C趋于平衡值且动力学可通过弛豫时间连续谱加以描述。可逆弛豫过程可用CSRO来说明,并且某一物理量的可逆变化并不意味着整个结构的变化是可逆的。     

FORMATION AND MAGNETIC PROPERTIES OF Dy2Fe17-xMnxC(x = 0-17) PREPARED BY ARC-MELTING

We report on alloys formed by replacing iron with manganese in the compound Dy₂Fe₁₇C_1.0 Samples were characterized by X-ray diffraction and magnetic measure-ments, The 2:17-type structure can be crystallized in the whole range of manganese substitution. The Curie temperature of the series of Dy₂Fe_17-xMn_xC_1.0(x= 0-17) drops down considerably from 515K for x = 0 to about 20K for compounds with high manganese concentration, and the compensation point was observed in a narrow range of x≈4-6. The rapid decrease of the magnetization shows that the manganese substitution is not a simple magnetic dilution to the transition-metal sublattice mo-ment, it indicates that the moment of Mn may be antiparallel to that of Fe. The field dependence of the magnetization of Dy₂Fe_17-xMn_xC_1.0 may indicate the existence of the nonlinear magnetic structure for the samples with high Mn conoentrations.     

Magnetic properties and in compound magnetocaloric effect PrFe12B6

Magnetic properties and magnetocaloric effect of compound PrFe12B6 are investigated. The coexistence of hard phase PrFe12B6 and soft phase α-Fe causes interesting phenomena on the curves for the temperature dependence of magnetization. PrFe12B6 experiences a first order phase transition at the Curie temperature 206 K, accompanied by an obvious lattice contraction, which in turn results in a large magnetic entropy change. The Maxwell relation fails to give the correct information about magnetic entropy change due to the first order phase transition nature. The large magnetic entropy changes of PrFe12.3B4.7 obtained from heat capacity method are 11.7 and 16.2 J/kg.K for magnetic field changes of 0-2 T and 0-5 T respectively.     

Effect of film thickness manganite-based on interfacial barrier of heterojunctions

Interracial barrier is a key factor that determines the performances of heterojunctions. In this work, we study the effect of manganite film thickness on the effective interracial barrier for La0.67Sr0.33MnO3/Nb：SrTiO3 junctions, The barrier is extracted from the forward current-voltage characteristics. Our results demonstrate that the barrier decreases gradually from -0.85 eV to -0.60 eV when the film thickness decreases from 150 nm to 2 nm. The overall value of the barrier is only about 50% of the corresponding one determined from the photovoltaic effect.