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通过X射线衍射分析和磁测量研究了Gd-Fe-Co-Cr四元系中对应于化学式Gd3(Fe,Co,Cr)29且Gd含量为一定值的截面内富Fe,Co区的相关系,重点探索了高Co含量3∶29型化合物合成的可能性,研究了3∶29型Gd3(Fe1-xCox)29-yCry化合物的结构与磁性.研究结果表明,获得3∶29型单相Gd3(Fe1-xCox)29-yCry化合物的范围为:y=5,0≤x≤0.7;y=5.5,0.7≤x≤0.8和y=6,0.8≤x≤0.9.基于对Gd3(Fe1-xCox)29-yCry化合物成相条件的研究,成功地合成了纯Co基Gd3Co29-yCry化合物,其固溶范围为6.5≤y≤7.3.3∶29型单相Gd3(Fe1-xCox)29-yCry化合物的晶体结构都属于单斜晶系,Nd3(Fe,Ti)29型结构,空间群为A2/m.得到3∶29型单相Gd3(Fe1-xCox)29-yCry化合物的固溶极限即Co含量的极大值与稳定元素Cr含量有关.Co原子的含量越高,所需稳定元素Cr的含量越大.值得注意的是,用Co原子替代Fe原子会导致Gd3(Fe1-xCox)29-yCry化合物磁晶各向异性的显著改变.当x≥0.4时,化合物的磁晶各向异性从易面型转变为易轴型. 相似文献
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通过X射线衍射分析和磁测量研究了Gd-Fe-Co-Cr四元系中对应于化学式Gd3(Fe,Co,Cr)29且Gd含量为一定值的截面内富Fe,Co区的相关系,重点探索了高Co含量3∶29型化合物合成的可能性,研究了3∶29型Gd3(Fe1-xCox)29-yCry化合物的结构与磁性.研究结果表明,获得3∶29型单相Gd3(Fe1-xCox)29-yCry化合物的范围为:y=5,0≤x≤0.7;y=5.5,0.7≤x≤0.8和y=6,0.8≤x≤0.9.基于对Gd3(Fe1-xCox)29-yCry化合物成相条件的研究,成功地合成了纯Co基Gd3Co29-yCry化合物,其固溶范围为6.5≤y≤7.3.3∶29型单相Gd3(Fe1-xCox)29-yCry化合物的晶体结构都属于单斜晶系,Nd3(Fe,Ti)29型结构,空间群为A2m.得到3∶29型单相Gd3(Fe1-xCox)29-yCry化合物的固溶极限即Co含量的极大值与稳定元素Cr含量有关.Co原子的含量越高,所需稳定元素Cr的含量越大.值得注意的是,用Co原子替代Fe原子会导致Gd3(Fe1-xCox)29-yCry化合物磁晶各向异性的显著改变.当x≥0.4时,化合物的磁晶各向异性从易面型转变为易轴型
关键词:
3(Fe1-xCox)29-yCry化合物')" href="#">Gd3(Fe1-xCox)29-yCry化合物
相关系和相结构
X射线衍射
磁晶各向异性 相似文献
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制备出具有室温单轴磁晶各向异性的非间隙型Co基Gd3Co29-xCrx化合物(x=65和70),x射线衍射和磁性测量表明所有单相化合物均属于单斜晶系,Nd3(Fe,Ti)29型结构和A2/m空间群.Gd3Co29-xCrx化合物的居里温度在x=65时为412 K,x=70时为359 K. Gd3Co29-xCrx化合物在x=65 时磁化强度随温度的变化曲线表明,在居里温度以下的某一温度处有一补偿点,在补偿点处求得晶格分子场系数nRT=33 T f.u./μB.
关键词:
Gd3Co29-xCrx化合物
x射线衍射
磁晶各向异性 相似文献
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通过x射线衍射分析和磁性测量对(Nd1-xErx)3Fe273Ti17化合物的结构与磁性进行了研究.单相(Nd1-xErx)3Fe273Ti17化合物的成相范围为x=00—05之间,所有化合物均属于单斜晶系、Nd3(Fe,Ti)29型结构和A2/m空间群.着Er含量的增加,(Nd1-xErx)3Fe273Ti17化合物的晶胞体积、居里温度TC和5K下的饱和磁化强度Ms均单调减小,而5K下的饱和磁化强度Ms和Er含量的关系与稀释模型所描述的结果相一致.(Nd1-xErx)3Fe273Ti1
关键词:
(Nd1-xErx)3Fe273Ti17化合物
磁晶各向异性
自旋重取向
磁相图 相似文献
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通过x射线衍射分析和磁性测量研究了RCo12-xTix(R=Y,Sm)化合物的结构与磁性,所有化合物全部具有ThMn12型结构.常规取向样品的x射线衍射谱表明,SmCo12-xTix化合物具有室温面磁晶各向异性,而YCo12-xTix化合物具有室温单轴磁晶各向异性.随着Ti含量的增加,SmCo12-xTix和YCo12-xTix化合物的居里温度TC及饱和磁化强度Ms均单调降低.YCo12-xTix化合物的磁晶各向异性场μ0Ha随Ti含量的增加而降低,而SmCo12-xTix化合物的磁晶各向异性场μ0Ha在x=1.74时出现一极大值,这可以用双次晶格模型来解释. 相似文献
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利用x射线衍射和磁测量研究了不同稳定元素Co以及Ti,V和Cr替代对Nd3Fe29-x-yCoxMy(M=Ti,V,Cr)化合物结构和磁性的影响.研究发现:每一个稳定元素都有一替代量极限,在此极限以内所有化合物均为Nd3(Fe,Ti)29型结构,A2/m空间群.不同稳定元素的溶解极限不同.Co的替代量与稳定元素有关,当以Cr作为稳定元素时,Cr的替代量随着Co含量的提高而提高,直到得到纯Co基3:29相化合物.Ti和V作为稳定元素时,Co原子的最大替代量分别为6.63和12.所有Nd3(Fe,Co,M)29(M=Ti,V,Cr)化合物在室温下均表现为平面各向异性.Nd3Fe26.8-xCoxV2.2的居里温度TC和饱和磁化强度Ms随着Co含量的增加而单调增加,自旋重取温度随Co含量增加而呈上升趋势,但在x=6处有一最小值,这可能与Co的择优占位有关;而Nd3Fe29-x-yCoxCry的居里温度和饱和磁化强度随着Co含量的增加先增加后降低,只在x=0和x=6处观察到自旋重取向现象. 相似文献
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合成了Er3Fe29-x-yCoxMy化合物(M=Cr,V,Ti,Mn,Ga,Nb)并用x射线衍射和磁测量等手段研究了它们的结构和磁性.发现Fe基Er3(Fe,M)29化合物结晶成哑铃对Fe-Fe无序替代的Th2Ni17型结构(P63/mmc空间群)而不能形成Nd3(Fe,Ti)29型结构,因此其化学式也可以用Er2-n(Fe,M)17+2n(n=0.2)表示.当Er3Fe29化合物中部分Fe原子被M原子所取代时,其居里温度均有一定程度的提高.所有Er3(Fe,M)29化合物在室温均为易面型各向异性.当Er3(Fe,M)29(M=Cr,V)中的部分Fe原子被Co原子取代且Co原子数与Fe原子数达到一定比值时,得到一个单斜结构的新相.磁测量表明Er3Fei95Co6V3.5在室温可能为单轴各向异性,在162K出现自旋重取向,其各向异性由易轴型变为易面型.在5K下于难磁化方向磁化时观察到一个一级磁化过程(FOMP). 相似文献
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利用x射线衍射和磁测量研究了不同稳定元素Co以及Ti,V和Cr替代对Nd3Fe29-x-yCoxMy(M=Ti,V,Cr)化合物结构和磁性的影响.研究发现:每一个稳定元素都有一替代量极限,在此极限以内所有化合物均为Nd3(Fe,Ti)29型结构,A2/m空间群.不同稳定元素的溶解极限不同.Co的替代量与稳定元素有关,当以Cr作为稳定元素时,Cr的替代量随着Co含量的提高而提高
关键词:
3(Fe')" href="#">Nd3(Fe
Co
29')" href="#">M)29
结构
磁性 相似文献
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合成了Er3Fe29-x-yCoxMy化合物(M=Cr, V, Ti, Mn, Ga, Nb )并用x射线衍射和磁测量等手段研究了它们的结构和磁性. 发现Fe基Er3(Fe,M)29化合物结晶成哑铃对Fe-Fe无序替代的Th2Ni17型结构(P63/mmc空间群)而不能形成Nd3(Fe,Ti)29型结构,因此其化学式也可以用Er2-n(Fe,M)17+2n (n=0.2)表示. 当Er3Fe29化合物中部分Fe原子被M原子所取代时,其居里温度均有一定程度的提高. 所有Er3(Fe,M)29化合物在室温均为易面型各向异性. 当Er3(Fe,M)29 (M=Cr, V)中的部分Fe原子被Co原子取代且Co原子数与Fe原子数达到一定比值时,得到一个单斜结构的新相. 磁测量表明Er3Fe19.5Co6V3.5在室温可能为单轴各向异性,在162K出现自旋重取向,其各向异性由易轴型变为易面型. 在5K下于难磁化方向磁化时观察到一个一级磁化过程(FOMP).
关键词:
稀土金属间化合物
晶体结构
磁晶各向异性 相似文献
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FORMATION AND MAGNETIC PROPERTIES OF NEW COMPOUNDS R3Fe29-xCrx(R=Y,Ce,Nd,Sm,Gd,Tb,and Dy) 下载免费PDF全文
A systematic investigation of structure and magnetic properties of the new R3Fe29-xCrx compounds(R=Y,Ce,Nd,Sm,Gd, Tb,and Dy)has been performed. The Curie temperature of R3Fe29-xCrx increased with increasing atomic number fromR=Ce to Gd and de creased from Gd to Dy. The saturation magnetization of R3Fe29-xCrx at 4.2 K decreased gradually with increasing atomic number from R=Y to Dy,except for Ce. The spin reorientations of the easy magnetization d irection were observed at around 230 K for Nd3Fe24.5Cr4.5 and 180 K for Tb3Fe28.0Cr1.0,and the magnetohistory effects were obser ved for Nd3Fe24.5Cr4.5 and Sm3Fe24.0Cr5.0 in a low field of about 0.04 T. First order magnetization process occurs in magnetic field of around 2.3 T at room temperature for Tb3Fe28.0Cr1.0. The saturation magnetization of Y3Fe27.2Cr1.8 at 4.2 K is 52.2μB/f.u., which corresponds to an average magnetic moment of 1.92μB per each Fe atom. 相似文献
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H. Oesterreicher F. T. Parker M. Misroch 《Applied Physics A: Materials Science & Processing》1977,12(3):287-292
Compounds RCo3B2 withR=Sm, Gd, and Er were prepared and identified structurally by X-ray diffraction. Magnetic properties of these materials were
studied down to liquid He temperature. The materials order ferromagnetically (e.g.,T
c
for GdCo3B2 is 58 K). The magnitude of saturation moments indicates that Co is nonmagnetic in this environment. Bulk specimens of the
compound SmCo3B2 show extraordinarily high coercive forces at 4.2 K (H
c
=50 kOe). The second-order crystal field term of Sm in this compound is calculated on the point charge crystal field model
and is found to be considerably larger than the one of Sm in SmCo5. This is mainly due to the unusual ratio of the lattice constants.
This work was supported by a grant from the National Science Fundation. 相似文献
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F. Pfuner L. Degiorgi K. Y. Shin I. R. Fisher 《The European Physical Journal B - Condensed Matter and Complex Systems》2008,63(1):11-16
We investigate the rare-earth polychalcogenide R2Te5 (R=Nd, Sm and Gd) charge-density-wave (CDW) compounds by optical reflectivity measurements. We obtain the optical conductivity
through Kramers-Kronig transformation of the reflectivity spectra. From the real part of the optical conductivity we then
extract the excitation energy of the CDW gap and estimate the fraction of the Fermi surface which is gapped by the formation
of the CDW condensate. In analogy to previous findings on the related RTen (n=2 and 3) families, we establish the progressive closing of the CDW gap and the moderate enhancement of the metallic component
upon chemically compressing the lattice. 相似文献
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Magnetic phase transition and the corresponding magnetostriction of intermetallic compounds RMnsGe2(R=Sm,Gd) 下载免费PDF全文
The temperature dependence of lattice constants a and c of intermetallic compounds RMn2Ge2 (R=Sm, Gd) is measured in the temperature range 10-800K by using the x-ray diffraction method. The magnetoelastic anomalies of lattice constants are found at the different kinds of spontaneous magnetic transitions. The transversal and longitudinal magnetostrictions of polycrystalline samples are measured in the pulse magnetic field up to 25T. In the external magnetic field there occurs a first-order field-induced antiferromagnetism-ferromagnetism transition in the Mn sublattice, which gives rise to a large magnetostriction. The magnitude of magnetostrictions is as large as 10-3. The transversal and longitudinal magnetostrictions have the same sign and are almost equal. This indicates that the magnetostriction is isotropic and mainly caused by the interlayer Mn-Mn exchange interaction. The experimental results are explained in the framework of a two-sublattice ferrimagnet with the negative exchange interaction in one of the sublattices by taking into account the lattice constant dependence of interlayer Mn-Mn exchange interaction. 相似文献
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The influence of interatomic distances on magnetic ordering in RMnSi compounds (R=La, Y, Sm, and Gd)
S. A. Nikitin T. I. Ivanova Yu. A. Ovchenkova M. V. Maslennikova G. S. Burkhanov O. D. Chistyakov 《Physics of the Solid State》2002,44(2):308-311
Magnetic ordering in the RMnSi (R=La, Y, Sm, and Gd) compounds is investigated. It is found that the type of magnetic ordering depends on the d Mn-Mn distance between manganese atoms inside the magnetic layers located in the planes perpendicular to the c axis. This inference is based on the results of studies performed with SmMnSi and GdMnSi compounds in which the distances between manganese atoms are close to the critical value d Mn-Mn that corresponds to the crossover between ferromagnetic and antiferromagnetic ordering in RMnSi compounds. The introduction of lanthanum and yttrium atoms into the rare-earth sublattice leads to an increase and a decrease in the unit cell size, respectively, and brings about magnetic phase transitions in the compounds under investigation. 相似文献