Kondo behaviour in magnetic (Ce−La)Pd2Si2

Susceptibility, specific heat and resistivity studies on CePd₂Si₂ and its pseudoternary system Ce_xLa_1–xPd₂Si₂ are reported. Replacement of Ce by La leads to a near dilution like decrease of the Néel temperaturesT _N (x): long range magnetic order in the ground state doublet exists in the wholex range explored (0.2x1). The present data indicate a concomitant Kondo effect, with Kondo temperaturesT _K decreasing linearly from 9 to 3 K, competing with the magnetic interaction. A close relationship between the value of the specific heat jump atT _N and the ratio between the two characteristic temperaturesT _N andT _K is demonstrated.     

57Fe Mössbauer spectroscopic and magnetic studies of R3Fe29-xVx (R=Y,Ce, Nd,Sm, Gd,Tb, and Dy)

Hyperfine Interactions - Mössbauer spectra for Fe atoms in the series of R3Fe29-xVx (R = Y, Ce, Nd, Sm, Gd, Tb, and Dy) compounds were collected at 4.2 K. The ratio of 14.5 T/μB between...     

Diffusion of Fe,Co, Nd,and Dy in R2(Fe1−xCox)14B where R=Nd or Dy

Transition metal and rare earth diffusion coefficients at 1323 K in Dy_2−yNd_y(Fe_1−xCo_x)₁₄B were determined by field emission energy dispersive spectroscopy compositional analysis of diffusion couple specimens. Various arrangements of component materials and temperatures were examined in order to understand the mechanisms affecting diffusion of the components and to predict the stability of functionally graded microstructures consisting of a dysprosium-rich (Dy_2−yNd_y(Fe_1−xCo_x)₁₄B) outer layer and a neodymium-rich (Nd₂(Fe_1−xCo_x)₁₄B) interior. Estimates of the mutual interdiffusion coefficients of Dy, Nd, Fe, and Co in this system were obtained from the preparation of arc melted and annealed polycrystalline specimens, assuming that the diffusion coefficients were independent of concentration (Grube solution). Fifteen diffusion couples were prepared and heat treated at 1323 K for various times in order to provide data for calculation of the diffusion coefficients. The results indicate that the diffusion coefficients of Fe and Co (D_Fe=3.28×10⁻¹⁰ cm²/s and D_Co=7.63×10⁻¹⁰ cm²/s) were significantly higher at 1323 K in this system than those for Dy and Nd (D_Nd=2.3×10⁻¹² cm²/s and D_Dy=2.9×10⁻¹² cm²/s).     

Effects of Co substitution on structural and magnetic properties of R3(Fe1−xCox)29−yVy (R=Tb,Dy)

Synthesis of two novel series of intermetallic compounds Tb₃(Fe_1−xCo_x)_27.4V_1.6 (x=0,0.1, 0.2, 0.3, 0.4) and Dy₃(Fe_1−xCo_x)_27.8V_1.2 (x=0, 0.1, 0.2, 0.3) with the monoclinic Nd₃(Fe,Ti)₂₉-type structure (3:29) is presented. In the Dy series for x=0.4 a disordered variant of the hexagonal Th₂Ni₁₇-type structure is formed. The cell parameters decrease and the Curie temperature increases with increasing of the Co content. In the case of the Tb₃(Fe_1−xCo_x)_27.4V_1.6 series in the M(T) curve a magnetic transition is observed which is attributed to spin reorientation phenomena. This critical temperature decreases with increasing Co from 473 K for x=0.1 to 393 K for x=0.3, and was not observed in the case of 0.4. XRD patterns of magnetically aligned powder samples reveal the presence of a tilted magnetic structure.     

FORMATION AND MAGNETIC PROPERTIES OF NEW COMPOUNDS R3Fe29-xCrx(R=Y,Ce,Nd,Sm,Gd,Tb,and Dy)

A systematic investigation of structure and magnetic properties of the new R₃Fe_29-xCr_x compounds(R=Y,Ce,Nd,Sm,Gd, Tb,and Dy)has been performed. The Curie temperature of R₃Fe_29-xCr_x increased with increasing atomic number fromR=Ce to Gd and de creased from Gd to Dy. The saturation magnetization of R₃Fe_29-xCr_x 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 Nd₃Fe_24.5Cr_4.5 and 180 K for Tb₃Fe_28.0Cr_1.0,and the magnetohistory effects were obser ved for Nd₃Fe_24.5Cr_4.5 and Sm₃Fe_24.0Cr_5.0 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 Tb₃Fe_28.0Cr_1.0. The saturation magnetization of Y₃Fe_27.2Cr_1.8 at 4.2 K is 52.2μ_B/f.u., which corresponds to an average magnetic moment of 1.92μ_B per each Fe atom.     

Photodetachment cross section of S^- in electric and magnetic fields＊

In this paper, the quantum-mechanical photodetachment cross section of S^- in uniform electric and magnetic fields at arbitrary angles is presented. It compares the quantum-mechanical cross section with the quantum source formalism cross section. The results show that at large angle, the two results have good agreements, however, with the decrease of the angles, they deviate obviously from each other. The reasons for this discrepancy are also discussed.     

Synthesis and characterization of layered perovskite-type oxides LnSr2MnFeO7 (Ln = La, Nd, Gd, and Dy)

Layered perovskite-type oxides LnSr₂MnFeO₇, with Ln?=?La, Nd, Gd, and Dy, have been synthesized by conventional solid-state reaction method. Rietveld refinement shows that all the phases were found to crystallize with tetragonal unit cell in the space group I4/mmm. The unit cell parameters a and c decrease monotonically with decreasing effective ionic radius of the lanthanide ion. The phases show insulating behavior with no anomalous features in the entire temperature range of 150–350 K and the electrical conduction occurs by Mott’s variable range hopping mechanism. The magnetic studies suggest that the phases are antiferromagnetic and the Weiss constant (θ) increases with decreasing ionic radius of lanthanide ion.     

Raman Active Phonons in RCoO3 （R=La, Ce, Pr, Nd, Sm, Eu, Gd, and Dy） Perovskites

We examine RCoO3 （R=La, Ce, Pr, Nd, Sin, Eu, Gd, and Dy） perovskites prepared with the solid-state reaction method by Raman spectroscopy, and report the Raman active phonons in the RCoO3 perovskites crystallized in cubic symmetry for RCoO3 （R=La, Ce, Pr and Nd） and orthorhombic symmetry for RCoO3 （R=Sm, Eu, Gd, and Dy）. It is found that the Raman spectra of RCoO3 perovskites are strongly dependent on the ionic radius of the rare earth elements, and the frequency shift of the most intense modes of the orthorhombic samples are correlated with some structural parameters such as Co-O bond distances, ionic radius of the rare earth elements and Jahn-Teller distortion. It is clear that Raman spectroscopy has the advantage of sensitivity to structure distortion and oxygen motion.     

The behaviour of superparamagnetic small particles in applied magnetic fields: A Mössbauer spectroscopic study of ferritin and haemosiderin

Small magnetically ordered particles display characteristic temperature dependent superparamagnetic behaviour in their Mössbauer spectra, as a result of the interplay between the thermal energy and the magnetic anisotropy energy of each particle. In the presence of an applied magnetic field there is an additional energy term arising from the net magnetic moment of the particles. The resulting Mössbauer spectra depend on the size of the anisotropy energy relative to the energy of the magnetic moment of the particles in the applied field. The present applied field Mössbauer measurements on ferritin and haemosiderin indicate that in these materials the anisotropy energy dominates, although the spectra can still be analysed to give information on the magnetic moment of the particles.     

Magnetic properties and magnetic structures of the CeScSi-type RMgPb (R=Ce–Nd,Sm, Gd–Tm) compounds

Investigations made by powder X-ray diffraction, magnetic measurements and neutron powder diffraction on the CeScSi-type ternary magnesium plumbides RMgPb (R=Ce–Nd, Sm, Gd–Tm) are reported. Macroscopic magnetic measurements performed in the 2–300 K temperature range show that these compounds follow a Curie–Weiss law in the paramagnetic state (except SmMgPb) and behave antiferromagnetically at low temperature (T_Ν≤61 K). Field dependence of the magnetization performed at 5 K evidence metamagnetic-like behaviors (H_crit<7 T). Neutron powder diffraction evidenced complex antiferromagnetic structures in fair agreement with the magnetic data. PrMgPb and NdMgPb compounds present a commensurate antiferromagnetic structure, while (Tb–Er)MgPb are characterized by incommensurate sine-wave modulated magnetic structure down to lower temperature or square-wave magnetic structure due to appearance of higher odd integer harmonics. CeMgPb and TmMgPb evidence more complex sine-wave modulated magnetic structures, never encountered with the CeScSi-type structure, characterized by two propagation vectors. These results are discussed and compared with those of the isotypic RMgSn compounds.     

Electronic structure and magnetic properties of RCo5−xMx (R=Y,Pr and M=Al,Si) system

Detailed theoretical and experimental investigations of the electronic and magnetic properties of the RCo_5?xM_x compounds (R=Y, Pr and M=Si, Al) have been performed. All theoretical investigations of the electronic and magnetic properties of the system have been done using the Korringa–Kohn–Rostoker (KKR) band structure method. The Si for Co substitution in RCo₅ does not change the magnetic ordering: the RCo_5?xSi_x with R=Y, Nd and Pr is ferromagnetic, whilst the heavy rare-earth containing compounds are ferrimagnetic. The important modifications induced by this substitution concerns the magnetic properties of the system: the Curie temperature and the magnetic moments of Co decrease with Si content, indicating the weakening of the Co–Co exchange interaction. The band structure calculations evidence the hybridization between the 3d electronic states of Co and the 3p states of Si as possible reason for the diminishing of Co–Co exchange interaction. Also, the volume effect on the magnetic properties of the YCo₄Si was investigated using theoretical methods. The results are compared with the experimental measurements in order to distinguish the origin of magnetization reduction in YCo₄Si compared with YCo₄Al.     

Structure and magnetism of the R2Fe14−xCoxB ferrimagnetic systems (R = Dy and Er)

R₂Fe_14−xCo_xB ferrimagnetic systems (R = Dy and Er) have been synthesized and studied by X-ray and magnetometry methods to determine the lattice parameters, Curie temperatures, saturation magnetizations, anisotropy fields and spin-reorientation temperatures. It has been established that the single phase materials, exhibiting a tetragonal crystal structure, can be formed in the Dy-based system only for x ⩽ 8, while in the Er-based system only for x ⩽ 5. An average increase of the Curie temperature of 58 K per one substituted Fe atom by Co is observed for both systems (x ⩽ 5). A characteristic maximum in composition dependence of the saturation magnetizations at 295 K is found for x ≃ 2, although this is less pronounced than in light rare earth-based Co-substituted systems. The composition dependencies of the anisotropy fields for the Dy-based system at 77 and 295 K show distinct maxima for low Co concentrations and a sharp decrease for higher Co content. The spin-reorientation temperature for the Er-based system is shifted towards higher temperatures by the Co substitution. A brief comparison between ferro- and ferrimagnetic R₂Fe_14−xCo_xB systems is included.     

Shift of proton magnetic shielding in ClH ··· Y dimers (Y = N2, CO,BF)

The change in the proton magnetic shielding constant of ClH on the formation of the linear hydrogen-bonded ClH?·?·?·?Y (Y?=?N₂,?CO,?BF) complexes was determined by GIAO ab initio computations at the B3LYP/aug-cc-pVQZ level of theory. The characteristic downfield shift of the isotropic proton magnetic resonance in the vibrationally red-shifted complexes (ClH?·?·?·?N₂, ClH?·?·?·?CO and ClH?·?·?·?BF) is significantly larger than in the blue-shifted complexes (ClH?·?·?·?OC and ClH?·?·?·?FB). These results are rationalized by considering the changes in the magnetic and electric contributions to the proton shielding in ClH.     

Structural and magnetic properties of Dy2Co17—xMnx compounds

Using x-ray diffraction and magnetic measurements, we have studied the structural and magnetic properties of Dy₂Co_17-xMn_x (x=0∽5) compounds with a rhombohedral Th₂Zn₁₇-type structure. With an increasing Mn concentration x, the unit-cell volume V was found to increase linearly. The Curie temperature T_c decreases linearly, and the saturation magnetization M_s at 5K first increases slightly for x<1, then decreases rapidly for x>1 with a further increase of Mn concentration x. In compounds for x=1～3, a spin reorientation was found. A magnetic diagram of the compounds is given.     

The Mechanism of 4f-5d hybridization in Sm1−x R x S (R=Ce, Gd, and Y) systems with intermediate valence

For Sm_1?x R _x S (R=Ce, Gd, Y) systems with intermediate valence, the population of Sm 4f states (valence) and populations of Ce 5d, Gd 5d, and Y 4d states are determined by the method of x-ray line displacement. It is found that, in all the systems under investigation, the valence of Sm upon transition to the intermediate valence state increases from m≈2.5 (x≈0.15–0.25) to m≈2.65 (x≈0.8) and then decreases. The populations of Ce, Gd, and Y d states remain nearly constant over the entire region of compositions: $\bar n_d = 0.78 \pm 0.03,0.43 \pm 0.04$ , and 1.07±0.04 for Ce, Gd, and Y, respectively. The experimental dependence of the Sm valence on the composition is explained under the assumption that the 4f electron of an Sm atom can be hybridized through two channels, namely, with the 5d electron of the neighboring Sm atom and with its own 5d electron.     

The magnetic phases and structures of Ce(Ru1-xFex)2Ge2 studied by μ-SR

We report on the structures of the magnetic phases of CeRu₂Ge₂ and their evolution in the series Ce(Ru_1-xFe_x)₂Ge₂. The crossover behavior between the ferromagnetic ground state of CeRu₂Ge₂ to the paramagnetic ground state of CeFe₂Ge₂ is compared to the behavior in the series CeRu₂(Ge_1-xSi_x)₂. A profound difference is observed between these two series, which is in contradiction to the uniform behavior predicted by the Doniach-necklace model. This revised version was published online in August 2006 with corrections to the Cover Date.     

Magnetic properties of single grain R–Mg–Cd primitive icosahedral quasicrystals (R=Y,Gd, Tb or Dy)

The growth and characterization of single grains of the primitive icosahedral quasicrystal R–Mg–Cd (R=Y, Gd, Tb or Dy) are described. From the thermodynamic properties, it is confirmed that the system is a spin glass exhibiting the characteristic spin-freezing transition of such systems. There is no evidence for two distinct freezing transitions previously observed for polygrain samples. The bulk magnetic properties and the effect of crystalline electric fields on the spin-freezing temperature are found to be very similar to those of the face-centred icosahedral quasicrystal R–Mg–Zn.     

Pulsed EPR spectroscopy of Gd3+ centers in Ca1−x R x F2+x (R=La, Y) mixed crystals

A study of Gd³⁺ centers in Ca_1?x R _x F_2+x (R=La, Y) crystals using pulsed EPR spectroscopy is presented. The echo-induced EPR (ESE-EPR) spectrum shows, besides the signal of slightly perturbed cubic Gd³⁺ centers, a broad signal at g≈2 due to Gd³⁺ centers at low symmetry sites. To describe the effects of R³⁺ ions on the EPR Gd³⁺, a model, including cubic and linear R³⁺?2F _i ^? centers, is developed. Its predictions are compared with the experimental results. The composition dependence of the EPR signal due to slightly perturbed cubic Gd³⁺ centers in mixed Ca_1?x R _x F_2+x crystals is explained taking into account the different clustering tendency in La and Y crystals. Moreover, the formation of mixed clusters involving R³⁺ and Gd³⁺ ions is proposed for both series of samples. A greater clustering trend is found in the Y crystals than in the La ones. Gd³⁺ ions are found to be a “non innocent” paramagnetic probe for structural studies in these mixed crystals.