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1.
W. Zarek M. Pardavi-Horvath Z. Obuszko 《Journal of magnetism and magnetic materials》1980,21(1):47-50
Results of magnetic investigations on Sm6Mn23-xFex compounds performed over a wide temperature range are presented. It was found that replacing the Mn atoms in Sm6Mn23 and Fe atoms in Sm6Fe23 by Fe and Mn, respectively, causes a rapid reduction in both the Curie temperature and the magnetic moment. No magnetic order was found in the 4 < x < 8 range. The temperature dependence of the reciprocal susceptibility of the investigated compounds can be described using the Néel law. 相似文献
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The structural and magnetocaloric properties of Mn1.35Fe0.65P1-xSix compounds are investigated. The Si-substituted compounds, Mn1.35Fe0.65P1-xSix with x = 0.52, 0.54, 0.55, 0.56, and 0.57, are prepared by high-energy ball milling and the solid-state reaction. The X-ray diffraction shows that the compounds crystallize into the Fe2P-type hexagonal structure with space group P62m. The magnetic measurements show that the Curie temperature of the compound increases from 253 K for x = 0.52 to 296 K for x = 0.56. The isothermal magnetic-entropy change of the Mn1.35Fe0.65P1-xSix compound decreases with the Si content increasing. The maximal value of the magnetic-entropy change is about 7.0 J/kg稫 in the Mn1.35Fe0.65P0.48Si0.52 compound with a field change of 1.5 T. The compound quenched in water possesses a larger magnetic entropy change and a smaller thermal hysteresis than the non-quenched samples. The thermal hysteresis of the compound is less than 3.5 K. The maximum adiabatic temperature change is about 1.4 K in the Mn1.35Fe0.65P0.45Si0.55 compound with a field change of 1.48 T. 相似文献
3.
F. Pourarian E.B. Boltich W.E. Wallace R.S. Craig S.K. Malik 《Journal of magnetism and magnetic materials》1980,21(2):128-132
R6Mn23 systems, with R = Gd, Ho and Er, were hydrided to the composition R6Mn23Hx where x ap; 22. Magnetic properties of these systems and the parent intermetallics were studied over the temperature range 4 to 300 K and at applied field up to 21 kOe. Since Y6Mn23H25 was established earlier to exhibit only Pauli paramagnetism, the magnetism of the R6Mn23 hydrides must originate with the rare earth sublattice. Gd6Mn23H22 orders at ≈ 150 K, whereas ordering in Gd6Mn23 occurs at 468 K. The moment measured at 4 K indicates a non-collinear structure, perhaps generated by competition involving exchange between nearest and next nearest neighbors. The hydrides involving Ho and Er appear to remain paramagnetic to the lowest temperatures studied, perhaps because the reduced de Gennes factor exchange is insufficient to produce magnetic ordering. The possibility cannot be excluded, however, that they are antiferromagnetic. 相似文献
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In this paper, we present our recent experimental results of magnetic and transport properties of Gd1−xLaxMn2Ge2 intermetallic compounds with the ThCr2Si2-type layered structure. The results obtained indicate that, in GdMn2Ge2, a first-order transition from a collinear antiferromagnetic to a collinear ferrimagnetic state appears with decreasing temperature at Tt3, below the Néel temperature TN. In Gd1−xLaxMn2Ge2 compounds with x=0.05 and 0.075, after ordering ferrimagnetically at Tt1, two kinds of first-order transitions from a canted ferrimagnetic to a non-collinear antiferromagnetic state and from a non-collinear antiferromagnetic to a reentrant canted ferrimagnetic state occur at Tt2 and Tt3. In Gd0.925La0.075Mn2Ge2, a field-induced metamagnetic transition from non-collinear antiferromagnetism to canted ferrimagnetism occurs at relatively low fields, accompanied by fractal like multi-step transitions, the so called “devil's stair-case”. Furthermore, a negative giant magnetoresistance (GMR) effect (Δρ/ρ15%) was observed at the field-induced metamagnetic transition. The mechanism of this negative GMR was clarified by comprehensive measurements of the resistivity on single crystals Gd0.925La0.075Mn2Ge2 and TbMn2Ge2. With further increasing x, only canted ferrimagnetism appears with a compensation temperature for 0.10<x<0.40, whereas no compensation behavior appears for x>0.50. The phase diagram obtained indicates that the overall magnetism is controlled by the Mn–Mn intralayer distance in the tetragonal c-plane, reflecting the two-dimensional arrangement of Mn atoms. 相似文献
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采用溶胶-凝胶方法成功制备了Sr的替代化合物Y1-xSrxCoO3 (x=0, 0.01, 0.05, 0.10, 0.15, 0.20), 系统地研究了20–720 K温度范围内Y1-xSrxCoO3的电阻率温度关系. 研究表明, 随着Sr的替代含量的增加, Y1-xSrxCoO3的电阻率迅速地降低, 这主要是由于载流子浓度的增加引起. 样品x=0和0.01在低于330和260 K的温度范围内, 电阻率与温度之间满足指数关系lnρ∝1/T, 获得导电激活能分别为0.2950和0.1461 eV. 然而, 实验显示lnρ∝1/T关系仅成立于重掺杂样品的高温区; 在低温区莫特定律lnρ∝T-1/4成立, 且表明重掺杂引入势垒, 导致大量局域态的形成. 根据莫特T-1/4定律拟合实验数据, 评估了局域态密度N(EF), 它随着掺杂量的增加而增加.
关键词:
热电材料
溶胶-凝胶
3')" href="#">YCoO3 相似文献
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利用固相反应烧结技术制备La0.1Bi0.9-xEuxFeO3系列化合物. 利用X射线粉末衍射进行物相鉴定和结构分析,确定了材料的相关系:x≤0.05,材料为R3c结构相;0.08≤x≤0.12,材料为赝R3c结构相;x≥0.15是Pbnm相,其中0.15≤x≤0.20区域Pbnm相存在畸变. 磁测量结果表明,材料具有弱铁磁性,对于x≤0.20材料,磁矩在x=0.12成分存在极值. 利用阻抗分析仪测量了室温介电常数随成分的变化关系.讨论了材料的结构与弱铁磁性和室温介电常数间的关系.
关键词:
0.1Bi0.9-xEuxFeO3')" href="#">La0.1Bi0.9-xEuxFeO3
X射线衍射
磁性
介电常数 相似文献
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针对NiS2-xSex系统在x=1.00附近发生的反铁磁量子相变,制备了一系列NiS2-xSex(x=0.96, 0.98, 1.00, 1.05, 1.10和1.20)多晶样品,对其结构、磁性质和电阻率进行了系统的观测.结果发现:样品磁化率-温度关系呈现典型的强关联电子系统特征;与铜氧化物超导体相类似,它们的电阻率-温度关系在很宽的温
关键词:
量子相变
反铁磁自旋涨落
2-xSex体系')" href="#">NiS2-xSex体系 相似文献
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In this paper the values of the crystalline-electric-field
parameters Anm for R2Fe17 and
R2Fe17H3 (R=Tb,Ho,Er) are evaluated by fitting
calculations to the magnetization curves measured on the single
crystal at several temperatures. The fitted Anm for
R2Fe17 are strikingly different from those for the
corresponding R2Fe17H3. The energy gaps between the
lowest four energy levels for Ho ions in Ho2Fe172 can be
reproduced by using the fitted Anm and exchange field
2μBHex, which estimated from the fit of the
temperature dependence of the spontaneous magnetization combined
with inelastic neutron scattering experiment. 相似文献
12.
Electrical resistivity measurements have been performed on the system Mn5?x,FexSi3 for the compounds x = 0,1,2,3,4 and 5 from 4.2 K to above room temperature. From the shape of the ρ(T) curves it can be inferred that the transition from antiferromagnetic to ferromagnetic ordering occurs in the concentration range 3 ? x ? 4; for Fe5Si3 and MnFe4Si3 the ρ(T) curves are characterized by a break in their slope, whereas for x = 1,2 and 3 a large minimum appears. Mn5Si3 exhibits two successive minima at 74 and 105 K. Magnetic susceptibility measurements for x = 1, 2 and 3 give confirmation of the Néel temperature for x = 1 and 2, whereas for x = 3 the behaviour is more complex. 相似文献
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J.J. Bara A.T. Pȩdziwiatr W. Zarek M. Pardavi-Horvath Z. Kucharski J. Suwalski 《Journal of magnetism and magnetic materials》1982,27(1):32-40
The new Sm6(Mn1-xFex)23(0?x?1.0) system hasbeen synthesized and investigated in a wide temperature range by the X-ray, magnetometric and Mössbauer effect methods. The X-ray studies show that the system forms solid solutions which are isostructural with the Th6Mn23 type crystal structure throughout the entire compositional range. Both Fe-rich and Mn-rich regions of the system are magnetically ordered and are separated from each other by the non-magnetically ordered 0.22?x?0.33 region. The substitution of Fe atoms for Mn atoms in the Mn-rivh region and similarly of Mn atoms for Fe atoms in the Fe-rich region decreases both the Curie temperature and the value of the magnetic moment per molecule. The temperature dependence of the reciprocal susceptibility obeys the Néel law. The Mössbauer absorption spectra reflect wide distributions of the 57Fe hyperfine interaction parameters, and disappearance of long range magnetic coupling of Fe atoms in the magnetically ordered x=0 to 0.22 composition range. 相似文献
16.
用X射线衍射和磁测量手段研究了Ni部分替代Fe对具有ThMn12结构的Rfe11.3Nb0.7(R=Gd,Tb,Dy,Ho,Er和Y)化合物的结构与磁性的影响.研究表明,Ni部分替代Fe不改变晶体结构,但引起了晶胞体积收缩.随着Ni含量的增加,居里温度TC迅速上升,而饱和磁化强度Ms则单调减小.Ni部分替代Fe还导致了Fe次晶格的轴各向异性的迅速降低和RF11.3Nb0.7(R=Tb,Dy,Er)化合物中自旋重取向温度Tsr的变化.Tsr与Ni含量的关系用晶场理论给出了定性的解释.
关键词: 相似文献
17.
在金属间化合物的结构演变中,原子尺寸因素起着重要的作用.由于密堆积效应,不同原子半径比的元素往往形成不同的结构.而自由电子填充于原子构成的晶体结构的间隙中,它对化合物的结构也有影响.基于组合结构化合物Ho2Ni7-xFex,结合原子尺寸与自由电子对晶体结构的不同影响,文章探讨一种单位体积内自由电子浓度的经验方法来判断Ho2Ni7-xFex化合物中两种异构体间的转变.随着Fe含量的增加,Ho2Ni7-xFex化合物先结晶成Gd2Co7型三方结构,然后结晶成Ce2Ni7型六方结构.利用Rietveld精修技术和磁测量,获得了化合物的晶体结构参数和饱和磁化强度.化合物晶胞常数随Fe含量增加而增加,饱和磁化强度则随之减少(dMs/dx=-2).分析结果表明,单位体积内自由电子浓度更高,化合物形成三方结构,反之则形成六方结构. 相似文献
18.
RFe2Zn20(R代表稀土元素)型稀土金属间化合物因其低稀土含量和良好的铁磁性,已成为铁磁材料的研究热点之一.添加第四组元对该系列化合物的晶体结构和材料性能会产生一定影响.利用晶格反演方法获得了一系列有效的原子间相互作用势,对三元RFe2Zn20和四元RFe2Zn20-xInx化合物进行原子级模拟计算.研究表明,随着稀土元素原子量的增加,三元体系的晶格参数和体积呈线性下降,第四组元引入与否对该线性关系无直接影响.第四组元In替代Zn时,择优占据16c晶位,占满16c后选择占据96g晶位,始终不占据48f晶位.择优占位的结论符合实验观测,并与晶格反演势分析的结果一致.
关键词:
原子间相互作用势
择优占位
晶体结构 相似文献
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