By U. Carow-Watamura, D. V. Louzguine (auth.), Y. Kawazoe, U. Carow-Watamura, J.-Z. Yu (eds.)
In the current quantity actual homes of ternary amorphous alloys are awarded. for every of the 385 alloy structures the information, e.g., on density and constitution, on thermal, mechanical, magnetic, electric and optical homes, in addition to on corrosion habit, are supplied in textual content, tables and figures. the information are released in 3 components, the current second half masking 122 alloy structures from B-Be-Fe to Co-W-Zr.
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Extra resources for Physical Properties of Ternary Amorphous Alloys. Part 2: Systems from B-Be-Fe to Co-W-Zr
Example text
1 General Description A magnetic material is magnetized by an external magnetic field. A magnetizing field (H) is connected with magnetic flux density (B). In the B = μrμ0H relationship μ0 is the permeability of free space (μ0 = 4π·107 Hm−1) and μr is relative permeability. Ferromagnetic materials have spins aligned parallel to each other forming magnetic domains. Antiferromagnetic materials have spins oriented in antiparallel way. Hysteresis loop or B-H loop of the magnetization curve showing dependence of the magnetic flux density (B) from magnetic field strength (H) is the most common plot for characterizing magnetic materials.
Wagner, H. L. Joshi: Z. Naturforsch. 20a (1965) 325. T. Cromer: J. Chem. Phys. 47 (1969) 4857. T. A. Liberman: J. Chem. Phys. 53 (1970) 1891. E. A. Stern, F. W. Lytle: Phys. Rev. Lett. 71 (1971) 1204. A. C. Hamilton, in: International Tables for X-ray Crystallography. ), Birmingem, 1974, Vol. 4, p. 1. J. Wagner: J Non-Cryst. Solids 31 (1978) 1. Y. Waseda: The Structure of Non-Crystalline Materials. McGraw-Hill: New York, 1980, p. 41. A. I. Svergun: Structure Analysis by Small-Angle X-Ray and Neutron Scattering.
The intensity measured by the electron detector (electron energy analyzer) has two components. The first component is caused by the electrons emitted directly to the detector. Another one consists of the electrons emitted into other directions and then scattered into detector. 7 Mössbauer Spectroscopy This technique (Fig. 4) uses the resonance absorption of γ rays with finely defined energies by atomic nuclei. It allows to probe very small changes in nuclear energy levels caused by changes in the nuclear environment.