Pressure effect on magnetic properties of RCo12B6 (R=Y,Ce) compounds

The effect of pressure on magnetic properties of YCo₁₂B₆ and CeCo₁₂B₆ was studied in temperature range 5–300 K at pressures up to 9 kbar. The Curie temperature T_C and spontaneous magnetization M_S decrease with pressure for both compounds. The decrease can be attributed mostly to the volume dependence of both, the Co magnetic moment and the exchange interactions. The hybridization of the p–d states as a consequence of small distances between the Co and B atoms can be one reason of the relatively low pressure effects (ΔT_C/Δp=?0.39±0.02 K/kbar, d ln M_S/dp=?0.0013±0.0002 kbar^?1) in YCo₁₂B₆. Higher volume sensitivity of magnetic properties of CeCo₁₂B₆ in comparison with YCo₁₂B₆ can be attributed to the pressure induced changes of the Ce f- and Co d-states.     

Electronic structure and magnetism of R(Fe,Si)12 (R = Y, Nd)

The newly developed full-potential linearized augmented plane wave (LAPW) and local orbitals (lo) based on standard APW methods are briefly introduced, and the structure and magnetic properties of R(Fe, Si)12 compounds (R = Y, Nd) are calculated using the method. The distribution of Si at different sites is analyzed based on total energy of one crystal unit with structure having been optimized. The characters of magnetic moments, total density of states (TDOS) and partial density of states (PDOS) for different crystal sites Si occupies are obtained and analyzed. The results show that the total magnetic moments of RFe10Si2 (R = Y, Nd) are larger than those of RFe10M2 (M = Ti, V, Cr, Mn, Mo and W) and the hybridization mechanism is seen as follows. Si(8j) reduce the magnetic moments of Fe at three sites, however, Si(8f) mainly reduce the magnetic moments of Fe(8i) and Fe(8j) atoms. The Curie temperature is markedly enhanced by the introduction of Si atoms according to spin fluctuation of DOS at Fermi level.     

Electronic structure and magnetism of RPdIn compounds (R=La, Ce, Pr, Nd)

RPdIn (R = La-Nd) compounds were studied by means of magnetic susceptibility, specific heat and photoelectron spectroscopy measurements. The results prove that CePdIn is an antiferromagnetic Kondo lattice with T_N below 1.7 K. The Pr-based indide remains paramagnetic down to 1.7 K, and the lack of any magnetic ordering may be due to the presence of a singlet as the crystalline electric field ground state or/and strong hybridization between Pr 4f states and Pd 4d states. In turn, NdPdIn exhibits ferromagnetism below about 26 K. In contrast to CePdIn, for the Pr- and Nd-based compounds any significant enhancement of the electronic specific heat coefficient was observed.     

Magnetic studies of RCo12B6 compounds (R=Y,Ce, Pr,Nd, Sm,Gd and Dy)

Magnetization of the RCo₁₂B₆ borides (R=Y, Ce, Pr, Nd, Sm, Gd and Dy), which crystallize in a rhombohedral structure of the SrNi₁₂B₆-type, has been measured in the temperature range 4.2–300 K. All compounds were found to order magnetically with Curie temperatures ranging from 154 to 177 K. Saturation moments at 4.2 K were found to be 6.5, 5.4, 8.4, 8.8, 6.8, 2.1 and 5.9μ_B/f.u. for R=Y, Ce, Pr, Nd, Sm, Gd and Dy, respectively. These results imply a ferromagnetic coupling of Co and rare earth moments for light rare earths and an antiferrimagnetic coupling for heavy rare earths in these compounds. A spin-compensation effect is observed in GdCo₁₂B₆ alloys at T_comp=46 and 72 K, respectively. Results suggest that in CeCo₁₂B₆ the Ce ion exists in the quadripositive state. It is clear that RCo₁₂B₆ materials are not of interest for permanent magnet applications.     

Y(Fe,M)12化合物的电子结构与磁性(M=Nb,Si)

采用新近发展的全势能线性缀加平面波((L)APW) 局域轨道(lo)和广义梯度近似(GGA)密度泛函方法计算了Y(Fe,M)12化合物(M=Nb,Si)的电子结构,得到了相应的总态密度和局域态密度,并分析了替代原子与替代晶位不同引起态密度的变化。根据计算结果预测的居里温度变化与实验结果基本一致。     

Magnetic properties of RM6Al6 (R = light rare earth,M = Cu,Mn, Fe)2

The systems RM₆Al₆ were studied by X-ray, magnetization and Mossbauer spectroscopy (⁵⁷Fe and ¹⁵¹Eu) measurements. The RCu₆Al₆ which crystallize in the f.c.c. NaZn₁₃ structure order ferromagnetically at low temperatures (T_c = 16KforR = Eu). The RMn₆Al₆ systems which crystallize in the rhombohedral Th₂Zn₁₇ structure order antiferromagnetically ($\text{T}{}_{\mathrm{<mtext>n</mtext>}}\text{= 25K for R = Nd}$and Eu). LaFe₆Al₆ has the NaZn₁₃ structure and orders antiferromagnetically at a relatively low temperature, 38K. The correlation of crystal structure and magnetic properties of these systems and those of RM₆Al₆ (R = heavy rare earth, tetragonal ThMn₁₂ structure) are discussed.     

Onset of magnetism in concentrated ternary alloys II: Laves phase compounds A(Fe1-xBx)2 (A = Y,Zr, U; B = Mn,Co and Al)

The onset of magnetism as a function of concentration and the magnetic properties of nine ternary Laves phase systems A(Fe_1-xB_x)₂ (A=Y, Zr, U; B=Mn, Co and Al) are discussed in terms of homogeneous and heterogeneous models based on the SEW model and the Landau theory of phase transition of second order. A significant influence of the nomagnetic elements Y, Zr and U upon the Fe magnetic moment substituted by Mn, Co and Al is observed. Low temperature freezing phenomena affect the magnetization process around the critical concentration x_c in Y and Zr compounds while they seem to be of minor importance for the U systems. Comparing the magnetic properties of these nine systems implies that the magnetization process becomes more homogeneous in the sequence of Y-, Zr- and U(Fe, B)₂ compounds. This - together with volume considerations and the different magnetovolume effects observed as well as susceptibility measurements lead to the suggestion that the Fe moment tends to become more delocalized as one proceeds from Y to U compounds as a consequence of the growing extent to which Y, Zr, U d-electrons are hybridized with the 3d electrons. Furthermore, U can be regarded as tetravalent in these Laves phase compounds, except UAl₂, in which presumably an admixture of U³⁺ and U⁴⁺ occurs.     

Local magnetic order in57Fe doped Y(Ce)Co4B

In order to monitor the peculiar temperature dependence of the magnetization of the compounds YCo₄B and CeCo₄B from an atomistic point of view, samples doped with 1%⁵⁷Fe were studied by Mössbauer spectroscopy. From the two Co-sites present in this structure (2c, 6i), only the latter were found to be equipped by Fe. In the case of the Y-compound, the change of direction of the easy axis of magnetization could be confirmed. The broad maximum observed for the magnetization of the Ce-compound is not reflected by the⁵⁷Fe hyperfine field.     

Magnetic behaviour of Y(Fe, M)2 compounds M = Al, Co, Rh, Ir

In Y(Fe, M)₂ compounds, the presence of Fe moments even at high M concentrations and the appearance of a percolation limit for the onset of long range magnetic order is typical. A dominance of the volume contribution to the isomer shift is obtained, indicating that for the Fe atoms charge transfers are of minor importance.     

The119Sn Mössbauer effect in RMn6Sn6 compounds (R=Gd,Y)

The magnetic properties of intermetallic compounds RMn₆Sn₆ (T=Gd and Y) have been investigated by¹¹⁹Sn Mössbauer effect measurements. The differences of the hyperfine field on both the Sn₁ and Sn₃ sites were small between GdMn₆Sn₆ and YMn₆Sn₆, while the Mn sublattice orders ferromagnetically for R=Gd and antiferromagnetically for R=Y. This result indicated that Mn moments order antiferromagnetically in the intra-plane of the Kagomè net in YMn₆Sn₆.     

3d magnetism in R2Fe14B compounds

An investigation of the magnetic properties of R₂Fe₁₄B compounds with R = Y, La, Ce, Gd, Lu and Th has been carried out. In all compounds the value of the Fe moment is in the range 2.0–2.2μ_B, close to that of metallic Fe. This shows that effects of electron transfer and hybridization are weaker than in binary R-Fe compounds. The variations of the Curie temperatures of the different compounds is interpreted in terms of the dependence of the magnetic interactions on distance and on R. In all compounds, except Th₂Fe₁₄B, the temperature dependence of the anisotropy exhibits a maximum at T/T_c ≃ 0.4. This effect is ascribed to competition between contributions from different Fe atomic sites and/or to a change in the crystal field interactions associated with the magnetovolume anomaly which occurs in R₂Fe₁₄B compounds below T_c.     

Magnetic and57Fe Mössbauer studies of intermetallic compounds R2 (Fe1−x−y Ni x Co y )17 (R=Y,Gd,Tb,x=0,0.10, 0.20,y=0,0.05, 0.10)

Mössbauer studies of R₂(Fe_1?x?y Ni _x Co _y )₁₇ showed that the transferred hyperfine field at Fe nuclei due to magnetic rare earth (R) atoms is about one Tesla. Magnetic moments of the R atoms were determined from magnetic measurements as μTb=8.52μB, μGd=6.22μB. The mixed substitution of Ni and Co for Fe leads to an increase of the ordering temperature. A slight preference occupancy for Fe was observed involving the dumbbell shaped f or c site. The substitution effects of Ni and Co on the hyperfine field of f or c site, the average hyperfine field and the average isomer shift were also discussed.     

Nd1.9M0.1Fe12Co2B,M = Ti or Hf as a material for permanent magnets

Magnetic properties (saturation magnetizations, anisotropy fields and Curie temperatures) of the alloys of the composition Nd_1.9M_0.1Fe₁₂Co₂B, with M = Ti and Hf are presented. All of the compounds crystallize in the tetragonal Nd₂Fe₁₄B structure. With substitution of Nd by Ti or Hf, the saturation moment and Curie temperature decrease, but the anisotropy fields, H_A, are found to increase significantly. Theoretical energy products are reduced from 65 to 63 MGOe when Nd is replaced by Ti or Hf to the extent of x = 0.1.     

Spin arrangements in R2Co14B compounds (R = rare earth)

R₂Co₁₄B compounds (R = Pr, Nd and Tb) have been studied for evidence of spin reorientation in the temperature range 4.2 K − 1100 K with the use of magnetometry technique. It has been established that Pr₂Co₁₄BandTb₂Co₁₄B undergo spin reorientations at temperatures 664 K and 795 K, respectively. These are axis-to-plane reorientations with increasing temperature. Nd₂Co₁₄B undergoes two spin transitions as temperature progresses: one at ∼ 34 K (cone-to-axis) and the second at ∼ 546 K (axis-to-plane). A diagram of spin arrangements observed in all existing R₂Co₁₄B compounds has been constructed.     

Mössbauer effect study of R2Fe14C (R=Dy and Er) compounds

The results of⁵⁷Fe Mössbauer effect measurements and magnetic studies performed on Dy₂Fe₁₄C and Er₂Fe₁₄C compounds are reported. The magnetic contributions of different iron sites are estimated and compared with those of corresponding boron compounds. The magnetic behaviour of the studied compounds is analysed in the molecular field approximation considering a two sublattices ferrimagnet.     

Magnetoresistivity of the Kondo-system (La,Ce)B6

The electrical resistivity of the Kondo system (La, Ce)B₆ has been measured in longitudinal and transversal magnetic fields up to 6 Tesla in the temperature range 0.04–20K. Corresponding to the strong increase of the resistivity with decreasing temperature the alloys show a very large negative magnetoresistivity with a Kondo temperatureT _K =1.05K and a Kondo magnetic fieldB _K =1.1 Tesla. The observed anisotropy of the resistivity due to the magnetic field direction cannot be explained well by existing theories.     

Hyperfine interactions in ultrafine amorphous Fe−M−B (M=Ni,Co) alloys

Ultrafine amorphous (Fe, Co, Ni) B powders have been prepared by a chemical reduction method. The influence of the Co and Ni atoms on the distribution of internal magnetic fields P(B_hf) has been investigated. The quadrupole splitting distribution P(QS) of ultrafine amorphous Fe−Ni−B powders has a form similar to that derived for the dense random packing of atoms.