The crystal structures of the tetrahedral cluster compounds GaNb(4)S(8) and GaTa(4)Se(8) were determined by single-crystal X-ray diffraction. They crystallize in the cubic GaMo(4)S(8) structure type (F3m), which can be derived from the spinel type by shifting the metal atoms off the centers of the chalcogen octahedra along [111]. Electrical resistivity and magnetic susceptibility measurements show that the electronic conduction originates from hopping of localized unpaired electrons (S = (1)/(2)) among widely separated Nb(4) or Ta(4) clusters, and thus these materials represent a new class of Mott insulators. Under high pressure we find that GaNb(4)S(8) undergoes a transition from the Mott insulating to a superconducting state with T(C) up to 4 K at 23 GPa, similar to GaNb(4)Se(8) and GaTa(4)Se(8). High-pressure single-crystal X-ray studies of GaTa(4)Se(8) reveal that the superconducting transition is connected with a gradual decrease of the octahedral distortion with increasing pressure. DFT band structure calculations show that weakly coupled cluster orbitals are responsible for a high density of states at the Fermi level. The correct insulating magnetic ground state for GaNb(4)S(8) with mu(eff) = 1.73 mu(B) is for the first time achieved by the LDA+U method using U = 6 eV and rhombohedral symmetry.
Electronic conduction in GaM4Se8 (M=Nb,Ta) compounds with the fcc GaMo4S8-type structure originates from hopping of localized unpaired electrons (S=1 / 2) among widely separated tetrahedral M4 metal clusters. We show that under pressure these systems transform from Mott insulators to a metallic and superconducting state with T(C)=2.9 and 5.8 K at 13 and 11.5 GPa for GaNb4Se8 and GaTa4Se8, respectively. The occurrence of superconductivity is shown to be connected with a pressure-induced decrease of the MSe6 octahedral distortion and simultaneous softening of the phonon associated with M-Se bonds.
Eu 0.83 Fe 4 Sb 12 , was synthesized by arc melting in homogeneous practically single phase form. From Rietveld refinement isotypism was derived with the LaFe 4 P 12 -͑skutterudite͒-type, space group Im 3 , No. 204. The refinement also served to determine the Eu content of xϭ0.83(2). Eu 0.83 Fe 4 Sb 12 orders magnetically below 84 K and isothermal magnetization measurements reveal a spontaneous magnetization reaching about 4.5 B /f.u. at 6 T. The electronic configuration of the Eu ion in this compound appears to be close to the 4 f 7 state, thus behaving almost divalently. From the measurements of transport coefficients, the figure of merit Z was evaluated as ZTϷ0.08 at room temperature. The most outstanding property of this compound, however, is the significant magnetoresistance of about 130% at Tϭ1 K for a magnetic field of 12 T but still 30% near room temperature.
151 Eu ͑and 57 Fe) high-pressure Mössbauer investigations on EuFe 2 P 2 reveal that the pressure-induced isostructural phase transition 3ՇpՇ9 GPa is accompanied by a continuous valence transition from Eu 2ϩ to Eu 3ϩ with the consequence of the disappearance of the Eu͑4 f ) sublattice moment. However, contrary to EuCo 2 P 2 we find in the high-pressure phase of EuFe 2 P 2 no magnetic moment on Fe. Volume-dependent band-structure calculations in both systems show that the formation of the 3d moment strongly depends on the position of the 3d states relative to the Fermi energy and that the filling of the 3d states in EuCo 2 P 2 is mainly caused by the P-3p electrons.The rare-earth (RE) transition metal ͑T͒ phosphides, RET 2 P 2 , crystallizing in the ThCr 2 Si 2 -type structure belong to an interesting class of materials in which structural instability is intimately connected with electronic and magnetic instabilities. These strong electron correlations lead to the formation of a large variety of ground states in this series. Depending on the type of RE and/or T, one observes not only different magnetic phenomena such as 4 f -sublattice magnetism (EuCo 2 P 2 ), 1 3d-sublattice magnetism (LaCo 2 P 2 ) 2 or magnetism of both sublattices (PrCo 2 P 2 ), 3 but also intermediate valent behavior (EuNi 2 P 2 ) 4 or even superconductivity (LaRu 2 P 2 ). 5 Essentially responsible for such a broad variety of properties is the ability of the ThCr 2 Si 2 structure to adapt to several elements with various atomic sizes resulting in extremely different lattice parameters. In fact, within the RET 2 P 2 series, there exists two extremely dissimilar P-P distances along the c axis resulting in two isostructural phases: ␣ phase for a large P-P distance (d P-P Ϸ2.8 Å͒ with a nonbonding P-P state; and  phase for a short d P-P Ϸ2.3 Å forming a P-P single bond state. 6 Structural phase transitions of first-and second-order between these phases can easily be induced by changing composition, 7 temperature, 8 or applying external pressure. 9 According to recent band-structure calculations on some RET 2 P 2 compounds such structural phase transitions strongly affect the electronic structure of these systems. 10 Towards understanding such an interplay in RET 2 P 2 systems, we have recently performed high-pressure experiments ( 151 Eu Mössbauer spectroscpopy and x-ray diffraction͒ on the magnetically ordered compound EuCo 2 P 2 . 11 In this system, antiferromagnetism is due to ordering of the Eu 2ϩ ͑ 8 S 7/2 ) sublattice moments (T N ϭ66.5 K͒ while the Co(3d) sublattice exhibits no magnetic moments. Here, high-pressure experiments demonstrated that the pressure-induced first-order structural ͑␣→͒ phase transition at pϾ3 GPa is connected with a sharp valence transition of Eu from magnetic Eu 2ϩ to a nonmagnetic Eu 3ϩ ( 7 F 0 ) state. As a consequence, the disappearance of the Eu(4 f ) sublattice magnetism is accompanied by a simultaneous appearance of Co(3d) sublattice magnetism with T N *ϭ260 K. 11 These experimental findings, however, rais...
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