Materials Literature
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Crystal structure parameter of Cr1−xMxAs (M=Ti, Fe, Co, and Ni; x≤0.1) have been precisely determined as a function of temperature from 77 to 320 K. Discontinuous changes of lattice parameters have been observed at a special temperature. By this temperature the Néel temperatures TN of Cr1−xMxAs have been determined be…
Extended x-ray-absorption fine-structure spectroscopy (EXAFS) has been used to determine the position of Zr within the unit cell of Sm2Co17. Induction-melted Sm2Co17:Zr ternary alloys, aged at 1180 °C, then quenched, consisted of intimately mixed H2:17 and R2:17 having Zr in solid solution as well some regions of R2:1…
Dynamic vector Preisach models of hysteresis are developed, and the identification problem for these models is posed. It is shown that some experimentally measured relaxation times can be used for the solution of the identification problem for the dynamic vector Preisach models. Moreover, it is shown that the identifi…
The effect of an additional amount of CaCl2 and the amount of NdCl3 to replace Nd2O3 on the characteristics of the washed Nd-Fe-B powder alloys, and the role of chlorides on the disintegration process have been investigated. CaCl2, CaO, and unreacted Ca surrounded Nd2Fe14B grains uniformly as the chloride amount excee…
The thermal conductivity of 17 alkali halides with the NaCl structure has been calculated. The deformation-dipole model has been used to calculate realistic phonon dispersion relations, which are used to solve the Boltzmann equation with the variational method. Many different trial functions and linear combinations ha…
Pressure effects on spin-flop transition temperature (Tsf) of Mn2−xCoxSb have been measured in order to study the nature of spin-flop phase transitions. The magnetic phase diagrams for Tsf versus concentration and for Tsf versus pressure have been determined. Tsf increases with increasing applied pressure (dTsf/dp=2.9…
The intrinsic coercivities Hc of Nd14DyxFe79−xB7 magnets, prepared by a powder metallurgical method, with an addition of Dy (x=2 at. %), reached 21 kOe. The intrinsic coercivity Hc was kept over 10 kOe when the heating temperature was 150 °C and the temperature coefficient α(Hc) = −0.35%/°C was in a temperature range…
Upon cooling, ${\mathrm{Ag}}_{0.6}$${\mathrm{NbS}}_{2}$ shows a transition near ${\mathit{T}}_{\mathit{c}}$=124 K from an Ag-disordered phase to an incommensurately ordered phase. From single-crystal x-ray-diffraction data, the cell parameters of the basic hexagonal unit cell are determined as a=3.355(1) \AA{} and c=1…
The $^{2}$E(D)\ensuremath{\rightarrow} $^{2}$${\mathit{T}}_{2}$(D) emission of substitutional ${\mathrm{Cu}}^{2+}$ in ZnO has been observed in the 3700--5800-${\mathrm{cm}}^{\mathrm{\ensuremath{-}}1}$ spectral range under 50-keV electron-beam excitation at cryogenic temperatures. The excitation mechanisms of this cath…
A photoemission investigation of Fe-Pd and Fe-Pt transition-metal alloys, using \ensuremath{\sim}50--150-eV synchrotron radiation, is presented. We consider in particular the spectral distribution of Fe states when approaching the dilute limit. By means of the Cooper minimum in the 4d and 5d photoionization cross sect…
Amorphous thin films of (1−x)BiFeO3-xPbZrO3 for x=0.1–0.9 have been prepared by the technique of rf sputtering and the effects of sputtering conditions and annealing at high temperatures on magnetic properties of such films have been studied through magnetization measurements. A sintered polycrystalline target was use…
The properties of NiFeX ternary films (X being Al, Au, Nb, Pd, Pt, Si, and Zr) have been studied for soft-film biasing of the magnetoresistive (MR) trilayer sensor. In general, the addition of the element X into the NiFe alloy film decreases the saturation magnetization Bs and magnetoresistance coefficient of the film…
The angular dependence of the coercive field Hc(ϑ) is discussed as a means of studying magnetization reversal in permanent magnets. We consider Hc(ϑ) for permanent magnets RFeB (R=Pr, Nd) for temperatures between 4.2 and 300 K. At high temperatures, it is found that Hc may increase by a factor 1.5–2 as ϑ increases fro…
Magnetic susceptibility studies of several A2CuBr4 salts, where A is an organoammonium cation, are reported. These salts contain tetrahedrally distorted CuBr2−4 anions. Magnetic exchange pathways exist through interanionic Br⋅⋅⋅Br pathways. In this manner, various types of new antiferromagnetic spin 1/2 magnetic syste…
The electronic structure of PtMnSb has been studied by means of the linear muffin-tin-orbital method of band-structure calculation. In agreement with earlier investigations a so-called half-metallic behavior has been found. Until now, this exotic feature of the band structure of PtMnSb, which is made responsible by so…
The crystal structure of fructose-1,6-bisphosphatase (EC 3.1.3.11) complexed with the product fructose 6-phosphate (F6P) has been refined at 2.1-A resolution to an R factor of 0.177 with root-mean-square deviations of 0.014 A and 2.9 degrees from the ideal geometries of bond lengths and bond angles, respectively. The…
We have examined incident-beam effects in electron-stimulated Auger-electron diffraction (AED) on a cleaved GaAs(110) surface. The results indicate that incident-beam diffraction is significant in an AED experiment, and that the dissipative nature of the incident beam in contributing to the Auger process must be accou…
In situ crystallized barium hexaferrite films have been deposited with a target-facing sputtering system under previously optimized conditions on four different substrates which are: SiO2, ZnO, Gd3Ga5O12, and Al2O3. By using several structural and magnetic characterizations different growth mechanisms were put forward…
We have imaged ten different superstructures on highly oriented pyrolytic graphite near adsorbed platinum particles using a scanning tunneling microscope. These superstructures are localized in small areas near the platinum particles and decay within a distance of 2--5 nm into the graphite lattice. When Fourier transf…
Thin Si films on thermally grown ${\mathrm{SiO}}_{2}$ layers were completely melted by pulsed-laser irradiation. The molten films cool very rapidly (>${10}^{9}$ K/s) until bulk nucleation initiates solidification. The quench rate was varied by changing the thickness of the Si or the ${\mathrm{SiO}}_{2}$ layers. For…