Peculiarities in the electron spectrum of superconducting laves phase ZrxHf1−xV2

Structurally unstable superconducting Laves phases Zr_xHf_1?xV₂ were investigated in the temperature range 4.2 – 300 K for temperature dependence of magnetic susceptibilities χ, resistivity ρ, and X-ray fluorescent emission 2K-spectra of vanadium. Anomalous dependences χ and ρ as compared to common metals was discovered below 150 K. This may be explained in terms of a phase transition of Peierl's type when the lattice instability results from the instability of the electron spectrum due to the dielectric slit that appears on flat parts of the Fermi surface. The presence of regions with localised electron density in the Laves phases on the low-energy side of the vanadium emission spectrum at low temperatures (T=10K) indicates an essential rebuilding in the electron spectrum of valence electrons.     

VSe2−xSx materials as battery cathode

The properties of the solid solution VSe_2?xS_x 0 ? x_nom ? 2 have been investigated for secondary battery application. The phase VSe₂ is observed for 0 ? x_nom ? 1.2 and the phase V₅S₈ is found using RX analysis for x_nom >1.2. The amount of lithium chemically incorporated in this structure by reaction with n-butyllithium is 2 Li/vanadium for 0 ? x_nom ? 0.8 and 1.4 Li/vanadium for V₅S₈. An electrochemical technique (galvanostatic) indicates that the amount of lithium incorporated depends on the x_nom values, the grain size and the discharge rate. The best results are obtained for 0.2 ? x_nom ? 0.6 (capacity = 164?172 Ah kg^?1 and energy density = 385?465 Wh kg^?1).     

EPR investigations of oxidation effects in (V1−xMox)2−δO3

Electron paramagnetic resonance (EPR) investigations has been carried out on the new family of molybdenum doped vanadium sesquioxides (V_1−xMo_x)_2−δO₃. The oxidation effects were monitored from the rate of paramagnetic V⁴⁺ created when the sample is exposed to the air. The effects of the oxidation time, sample temperature, and annealing at 1000 °C under a diluted hydrogen atmosphere on the EPR signal features are analyzed. The V⁴⁺ concentration in the oxidized samples is determined and the relaxation effects driven by the conduction electrons are pointed out from the thermal behaviour of the EPR line features. EPR spectra of all the oxidized samples also reveal a small ferromagnetic contribution strongly correlated with the V⁴⁺ content.     

A survey on the effect of vanadium content on the magnetoelastic properties of YFe12−xVx alloys

Experimental results on the thermal expansion and magnetostriction of YFe_12−xV_x (1.5≤x≤3.5) alloys are reported. The results show that the anisotropic magnetostriction (Δλ) at a finite field (1.5 T) increases with increasing vanadium content in the range of x<2. But for x>2, a decrease in the magnetic anisotropy with increasing vanadium content causes a decrease in the saturation values of Δλ. In addition, the thermal expansion coefficient becomes a minimum for x≈2. Experimental curves exhibit that the forced volume magnetostriction (ΔV/V) is positive and increases linearly with the applied field at high fields. But in the low field region (≤0.5 T), a minimum appears in the isothermal curves of ΔV/V around the saturation field. The results are explained by considering the influence of vanadium content on the magnetization anisotropy of YFe_12−xV_x compounds.     

Electronic conductivity and thermopower of Ca2NaMg2V3O12−x garnet

Results are reported from conductivity and thermoelectric power measurements on partially reduced Ca₂NaMg₂V₃O_12?x, with x < 5.10^?2, at temperatures of 300–1100 K. The conductivity is thermally activated with activation energies 0.26 ? E_a ? 1.28 eV for differently reduced samples. The thermopower is temperature independent in the 300–800 K region. These results are shown to be consistent with the adiabatic hopping of small polarons localised on the vanadium sublattice, where defect interactions result in the formation of multiple conduction pathways.     

Ferromagnetism of MnxLiyZn1−x−yO films

We had prepared Mn-doped ZnO and Li, Mn codoped-ZnO films with different concentrations using spin coating method. Crystal structure and magnetic measurements demonstrate that the impurity phases (ZnMnO₃) are not contributed to room temperature ferromagnetism and the ferromagnetism in Mn-doped ZnO film is intrinsic. Interesting, saturated magnetization decreases with Mn or Li concentration increase, showing that some antiferromagnetism exists in the samples with high Mn or Li concentration. In addition, Mn_0.05Zn_0.95O film annealed in vaccum shows larger ferromagnetism than the as-prepared sample and more oxygen vacancies induced by annealing in reducing atmosphere enhance ferromagnetism, which supports the bound magnetic polaron model on the origin of room temperature ferromagnetism.     

The ESR study of single crystal spinel ZnCr2Se4 diluted with Sb and V

The single crystal of Sb³⁺ and V³⁺ doped zinc chromium selenide spinel ZnCr₂Se₄ were prepared by a chemical transport method and characterized by ESR spectroscopy in order to examine the effect of nonmagnetic antimony and magnetic vanadium on properties of the system. For antimony admixtures the Neel temperature is very similar to that of the parent spinel ZnCr₂Se₄ (22 K). However, upon incorporating vanadium ions, the T_N temperature decreases down to 17.5 K, determined for the maximum vanadium content (x=0.06). The temperature dependence of the ESR linewidth over paramagnetic region is interpreted by an occurrence of spin-phonon interaction. The strong broadening linewidth together with its strong temperature dependence for vanadium doped ZnCr₂Se₄ is explained by the complex paramagnetic relaxation model.     

Room-temperature ferromagnetism in Zn1−xMnxO

In view of recent controversies on above room-temperature ferromagnetism (RTFM) in transition-metal-doped ZnO, the present paper aims to shed some light on the origin of ferromagnetism by investigating annealing effects on structure and magnetism for polycrystalline Zn_1−xMn_xO powder samples prepared by solid-state reaction method and annealed in air at different temperatures. Magnetic measurements indicate that the samples are ferromagnetic at room temperature (RTFM). Room temperature ferromagnetism has been observed in the sample annealed at a low temperature of 500 °C with a saturated magnetization (M_s) of 0.159 emu/g and a coercive force of 89 Oe. A reduction in RTFM is clearly observed in the sample annealed at 600 °C. Furthermore, the saturation magnetic moment decreases with an increase in grain size, suggesting that ferromagnetism is due to defects and/or oxygen vacancy confined to the surface of the grains. The experimental results indicate that the ferromagnetism observed in Zn_1−xMn_xO samples is intrinsic rather than associated with secondary phases.     

Magnetic studies of Hg1−xMnxS and Hg1−xMnxSe solid solutions

The magnetic susceptibility of Hg_1?xMn_xS and Hg_1?xMn_xSe solid solutions with 0.05 ≤x≤0.35 in the temperature range 1.2 K ≤ T ≤ 250 K is presented. The θ_p < 0 has been found. The critical temperature determined from the curve with two slopes is compared with the one obtained from EPR measurements. Two mechanisms of magnetic spin behaviour are considered.     

Electrical and optical properties of GexFexSe100−2x chalcogenide thin films

Optical absorption at room temperature and electrical conductivity at temperatures between 283 and 333 K of vacuum evaporated Ge_xFe_xSe_100−2x (0≤x≤15) amorphous thin films have been studied as a function of composition and film thickness. It was found that the optical absorption is due to indirect transition and the energy gap increases with increasing both Ge and Fe content; on the other hand, the width of the band tail exhibits the opposite behavior. The optical band gap E_opt was found to be almost thickness independent. The electrical conductivity show two types of conduction, at higher temperature the conduction is due to extended states, while the conduction at low temperature is due to variable range hopping in the localized states near Fermi level. Increasing Ge and Fe contents were found to decrease the localized state density N(E_F), electrical conductivity and increase the activation energy for conduction, which is nearly thickness independent. Variation of the atomic densities ρ, molar volume V, glass transition temperature T_g cohesive energy C.E and number of constraints N_Co with average coordination number Z was investigated. The relationship between the optical gap and chemical composition is discussed in terms of the cohesive energy C.E, average heat of atomization and coordination numbers.     

Magnetic behavior of Cd1−xMnxSe

We report EPR and magnetic susceptability measurements in single crystals of Cd_1?xMn_xSe as a function of concentration and temperature. The data indicate that there is a critical concentration x≈0.22 which we identify with the percolation critical point x_c.     

Magnetic properties of Fe1−xCoxO

Measurements are reported for the magnetic susceptibility of solid solutions Fe_1-xCo_xO for compositions with x =0.10 to 0.95 and for the temperature range 4.2 to 600 K. It is found that the Curie-Weiss law is obeyed at high temperatures while the dependence of the susceptibility and transition temperature on composition appear to be in good agreement with the “virtual crystal” approximation.     

Electrical resistivity and thermal conductivity of UP1−xSx

UP, US, and their solid solutions of several compositions were prepared, and the electrical resistivities of these samples were measured from liquid nitrogen temperature to 1000 K and the thermal diffusivities from 300 to 1000 K. It was shown that the resistivity of UP_1?xS_x at the paramagnetic region arose mainly from the scattering of conduction electrons by disordered spins localized at uranium ion sites. The resistivity of UP_0.4S_0.6 showed another anomaly below the transition temperature. A gentle hump of the thermal diffusivity of UP was observed at about 650 K. This was concluded to be due to the anomalous negative temperature coefficient of electrical resistivity observed above the Néel temperature up to about 550 K. The composition dependence of thermal conductivity of UP_1?xS_x was compared with that of UC_1?xN_x by separating the total conductivity into electronic and phonon contributions.     

Specific heat of diluted ferromagnets EuxSr1−xS

The specific heat C of diluted Eu_xSr_1?xS with Eu concentrations x = 0.95, 0.80, 0.70 and 0.60 was measured within the ferromagnetic regime. Both the temperature dependence of the magnetic part C_M and its behavior near the Curie temperature T_c show a variation with concentration which demonstrates clearly a change in magnetic behavior near x = 0.70. Eu_0.60Sr_0.40S exhibits properties which are more similar to spin glasses in spite of the long-range ferromagnetic order observed in the temperature range of measurement. This transient behavior is found to be consistent with previous observations.     

Magnetic behaviour of Sm6Mn23−xFex compounds

Results of magnetic investigations on Sm₆Mn_23-xFe_x compounds performed over a wide temperature range are presented. It was found that replacing the Mn atoms in Sm₆Mn₂₃ and Fe atoms in Sm₆Fe₂₃ by Fe and Mn, respectively, causes a rapid reduction in both the Curie temperature and the magnetic moment. No magnetic order was found in the 4 < x < 8 range. The temperature dependence of the reciprocal susceptibility of the investigated compounds can be described using the Néel law.     

Band structure of GaxIn1−xP alloys

An example of a systematic study of band structrue of alloys by electroreflectance technique is presented. Preliminary experimental analysis of lineshape convinced us of the good fitting of the three points method at room temperature. Electroreflectance spectra were measured at room temperature in the whole range of composition. The variations of E₀, E₁, E'₀, E₂ energies with composition are reported and compared with results of band structure calculation by the dielectric two bands method including the effect of disorder. The Γ-X crossover point is accurately determined. Inversely, electroreflectance technique is shown to be an interesting method for determining the composition of the alloys and to control macroscopic homogeneity.     

Exchange-inversion interaction and acoustical magnon soft mode in Mn2-xCrxSb

A magnon soft mode in Mn_2-xCr_xSb in the vicinity of the Brillouin zone boundary in c¹ direction, for the first order antiferro-ferrimagnetic phase transition, and the magnetization curve of the antiferromagnetic phase were measured. It was found that the soft mode energy squared is a linear function of temperature over a wide temperature range below and above the phase transition point.     

Dielectric anomaly in amorphous Si100-xAux system

In amorphous Si_100-xAu_x system the dielectric constant is decreasing with increasing frequency or with decreasing temperature at $\text{x ? 5.5\%}$. This is explained by considering the dispersion of the variable range hopping contribution to the dielectric constant. The dielectric constant at sufficiently high frequency or at sufficiently low temperature is increasing rapidly with increasing x in the region x ? 5.5%, which predicts the occurrence of the nonmetal-metal transition.     

Influence of hydrogen absorption on magnetic properties of Zr(Fe1−xVx)2 ternaries

Measurements of magnetization, susceptibility and Mössbauer effect were made on Zr(Fe_1?xV_x)₂ ternaries and their hydrides. Absorbed hydrogen leads to a large increase (20–30%) in volume without a change in the crystal structure. Ferromagnetism in the Fe-rich region is enhanced by hydrogen absorption, whereas hydrogenation leads to suppression of superconductivity in the V-rich range. The Fe moments in the Zr(Fe_1?xV_x)₂ hydrides are remarkably larger than those in the corresponding host compounds. The Fe moment in the β-ZrFe₂ hydride extrapolated reaches to 2.9μ_B, which exceeds the saturation value in bcc Fe. The hyperfine fields of ⁵⁷Fe in both Zr(Fe_0.8V_0.2)₂ and the hydride distribute widely, indicating that the Fe moments are very sensitive to the local environment arround the Fe atoms. Arguments are presented that it is possible to interprete the Fe moment increase by hydrogenation in terms of a decrease in occupancy of the 3d-band state due to electron transfers from Fe to hydrogen and/or vanadium.     

Magnetocaloric effect of GdCo2−xAlx compounds

The structure, magnetic property and magnetocaloric effect of GdCo_2−xAl_x (x=0, 0.06, 0.12, 0.18, 0.24, 0.4) compounds have been investigated by X-ray diffraction (XRD) and magnetic measurement techniques. The experimental results show that the GdCo_2−xAl_x (x≤0.4) compounds are single phase with a Laves-phase MgCu₂-type structure. The Curie temperature T_c initially increases, and then decreases with increasing Al content. The maximum value of T_c, 418 K, is reached for the compound with x=0.06. The magnetic entropy change, which is determined from the temperature and field dependence of the magnetization by the Maxwell relation, decreases almost linearly with increasing Al content.