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[en] Exchange and crystal fields (CF) acting on R³⁺ ions in R₂Fe₁₄B were investigated by means of inelastic magnetic neutron scattering. Experimental data for R=Pr, Nd, Gd, Tb, Dy, Ho, Er, and Tm are reviewed. Molecular fields H acting on R ions are calculated using neutron-scattering data for the CF models proposed earlier for these compounds based on single-crystal magnetization measurements. For Gd₂Fe₁₄B the molecular field acting on the Gd³⁺ ions was directly determined by inelastic neutron scattering as 2μ_BHm/k_B = 435 K

[en] For a group of s-, p-, and d-metal diborides (MB₂, where M = Mg, Al, Sc, Ti, V, Y, Zr, Nb, or Ta), variations in the cohesive energy and the formation energy in the presence of cation vacancies (MB₂ → M_0.75B₂), as well as the formation energy of cation-site vacancies, are analyzed using the FLMTO-GGA full-potential approach. The cationic nonstoichiometry for MB₂ phases is achievable only when they are prepared under nonequilibrium conditions

[en] This paper describes a method for the formation of complex boride whiskers within a final metal matrix. The complex boride comprises boron and at least two of the elements selected from the group consisting of Ti, Zr, Hf, V, Nb, Ta, Cr, Mo and W

[en] Magnetic and structural behaviour and phase relationships of materials of composition R³Ni⁷B² (R = Nd-Lu) were investigated. Detailed X-ray analysis yields that two hexagonal structures are encountered. For the heavy rare earth (Gd-Lu) the compounds crystallize in the CeNi³ structure. The space group is P6³/mmc and each unit cell contains two formula units. The R³Ni⁷B² where R = Nd-Sm (including Yb³Ni⁷B²) crystallize in the CeCo⁴B structure. The space group is P6/mmm and each unit cell contains one formula unit. The detailed crystal structures are discussed. The magnetic measurements show that Yb³Ni⁷B² and Lu³Ni⁷B² are Pauli paramagnetic. Sm³Ni⁷B² is ferromagnetically ordered with a huge intrinsic magnetic hardness. The magnetization at the coercive field at low temperatures is extremely time dependent. The R³Ni⁷B² which crystallize in CeNi³ structure are antiferromagnetic at low temperatures. All Mossbauer and magnetization experimental results can be explained assuming an antiferromagnetic exchange interaction in both 2(c) and 4(f) crystallographic sites and a ferromagnetic interaction between these sites. (author)

[en] An investigation of the interplay between long-range magnetic order and superconductivity in pseudoternary Ho(Rh/sub 1-x/Ir/sub x/)₄B₄ and Dy(Rh/sub 1-x/Ir/sub x/)₄B₄ systems was carried out by means of low temperature specific heat measurements. The properties of the intermediate valent compounds CeT₃B₂ and UT₃B₂ (T = CO, Ru, Rh, and Ir), as well as the behavior of superconductivity and ferromagnetism in pseudoternary Ce(Ru/sub 1-x/Rh/sub x/)₃B₂ compounds, were characterized by low temperature specific heat, electrical resistivity, and magnetic measurements. A low temperature phase diagram vs alloy composition was determined for Ho(Rh/sub 1-x/Ir/sub x/)₄B₄. The specific heat features associated with long-range ordering of the Ho⁺³ magnetic moments suggest mean field theory ferromagnetism for x less than or equal to 0.2. Antiferromagnetic ordering was observed for x greater than or equal to 0.2 and antiferromagnetic spin wave behavior was found for the ordered Ho⁺³ moments for x greater than or equal to 0.5. Unusual magnetic ordering occurs for 0.275 less than or equal to x less than or equal to 0.4 including two distinct magnetic transitions. The compound CeRh₃B₂ exhibits ferromagnetic ordering for T less than or equal to 113 K with a saturation magnetic moment 0.37 μ/sub B/ per formula unit, while CeRu₃B₂ exhibits superconductivity below 0.68 K. Values of the electronic specific heat coefficient γ for the compounds range from 9.7 mJ/mol-K² for CeCo₃B₂ to 64 mJ/mol-K² for UIr₃B₂. A phase diagram of the transition temperatures vs alloy composition was determined for Ce(Ru/sub 1-x/Rh/sub x/)₃B₂. Superconductivity of CeRu₃B₂ disappears for Rh substitution x greater than or equal to 0.38

[en] The present work deals with the high-temperature thermoelectric properties of transition metal [eg V, Cr, Mn, Ni, Cu] and lanthanide [e.g. Sc, Y, Gd, Er, Dy]-borides. In particular, intercalation compounds of beta-rhombohedral boron, compounds of the type MB_6_6, dodecaborides and hexaborides were examined. In the case of intercalation compounds of beta-rhombohedral boron it was found that the incorporation of metals such as Sc, Mn or Cu result in favorable thermoelectric properties. The reason is most likely the preferred occupation of the metal position M2 instead of M4. Composites, for example, DyB_6_6-DyB_1_2 show high electrical conductivities, high Seebeck effects at high temperatures due to the presence of DyB_1_2 and low thermal conductivities as a result of the DyB_6_6 matrix. At 1100K the composite DyB_6_6-DyB_1_2 shows a ZT value of 0.55, thus exceeding the ZT of boron carbide (B_1_3C_2) at this temperature which is considered the best p-type boride material. A composite of ErB_1_2-ErB_4-ErB_2 has negative Seebeck coefficients and shows a ZT value of 0.5 at 840K. Furthermore, the structure of tetragonal Scandiumdodecaboride ScB_1_2 was solved on the basis of synchrotron data from a crystalline powder, after it has been debated for decades but never fully resolved.

[en] We have performed accurate ab initio total energy calculations using the full-potential linearized augmented plane-wave (FP-LAPW) method with the generalized gradient approximation (GGA) for the exchange-correlation potential to systematically investigate elastic properties of 18 stable, metastable and hypothetical hexagonal (AlB₂-like) metal diborides MB₂, where M = Na, Be, Mg, Ca, Al, Sc, Y, Ti, Zr, Hf, V, Nb, Ta, Cr, Mo, W, Ag and Au. For monocrystalline MB₂, the optimized lattice parameters, independent elastic constants (C_ij), bulk moduli (B) and shear moduli (G) are obtained and analyzed in comparison with the available theoretical and experimental data. For the first time, numerical estimates of a set of elastic parameters of the polycrystalline MB₂ ceramics (in the framework of the Voigt-Reuss-Hill approximation), namely bulk and shear moduli, compressibility (β), Young's modulus (Y), Poisson's ratio (ν) and Lame coefficients (μ, λ), are performed.

[en] Borides Ln₂Ni₁₅B₉, where Ln=Y, Tb, Dy, Er, Tm, Yb, Lu, have been prepared for the first time. Their structure belonging to Ho₂Ni₁₅B₉ type is ascertained by the method of X-ray analysis

[en] Powder samples and single crystals of the Ti₉M₂Ru₁₈B₈ (Cr, Mn, Co, Ni, Cu, Zn) phases were synthesized from the elements and characterized by powder and single-crystal X-ray diffraction as well as energy-dispersive X-ray analysis. The new phases are all isotypic and crystallize in the tetragonal system as substitutional variants of the Zn₁₁Rh₁₈B₈-type structure (space group P4/mbm, no. 127). M₂ dumbbells are observed and interconnect to each other along the [001] direction to build ''ladders''. The M-M dumbbell distances vary from 2.48 to 2.50 A and the distances between two dumbbells (M₂.. M₂) are all close to 2.97 A, whereas the chains are well separated from each other by distances of at least 11.20 A. A strong variation of the unit cell volume with increasing valence electron count is observed in the series. According to the results of tight-binding electronic structure calculations, Ru-B and Ti-Ru contacts are responsible for the structural stability of these phases. The strength of the M-M and M-Ru interactions decreases with increasing valence electron count in the series. Non vanishing density of states at the Fermi level indicates metallic character for all phases. (orig.)