Magnetic Properties of Layered Transition Metal Compounds

Magnetic Properties of Layered Transition Metal Compounds
Author: L.J. de Jongh
Publisher: Springer Science & Business Media
Total Pages: 430
Release: 2012-12-06
Genre: Science
ISBN: 9400918607

In the last two decades low-dimensional (low-d) physics has matured into a major branch of science. Quite generally we may define a system with restricted dimensionality d as an object that is infinite only in one or two spatial directions (d = 1 and 2). Such a definition comprises isolated single chains or layers, but also fibres and thin layers (films) of varying but finite thickness. Clearly, a multitude of physical phenomena, notably in solid state physics, fall into these categories. As examples, we may mention: • Magnetic chains or layers (thin-film technology). • Metallic films (homogeneous or heterogeneous, crystalline, amorphous or microcristalline, etc.). • I-d or 2-d conductors and superconductors. • Intercalated systems. • 2-d electron gases (electrons on helium, semiconductor interfaces). • Surface layer problems (2-d melting of monolayers of noble gases on a substrate, surface problems in general). • Superfluid films of ~He or 'He. • Polymer physics. • Organic and inorganic chain conductors, superionic conductors. • I-d or 2-d molecular crystals and liquid crystals. • I-d or 2-d ferro- and antiferro electrics.

Electronic and Magnetic Properties of Amorphous Fe--P--B Alloys. [75 to 83 At. % Fe].

Electronic and Magnetic Properties of Amorphous Fe--P--B Alloys. [75 to 83 At. % Fe].
Author:
Publisher:
Total Pages:
Release: 1976
Genre:
ISBN:

The ternary diagram of the amorphous phase in the splat-cooled Fe--P--B system was investigated by x-ray diffraction measurements. Alloys were found to be amorphous within the Fe concentration range 75 less than or equal to c/sub Fe/ less than or equal to 83 at. percent. For a fixed Fe concentration, B substitutes for P over a large scale, the maximum substitution occurring for c/sub Fe/ = 80 at. percent. Concentration dependence of the electronic and magnetic properties was systematically studied in alloys within the whole amorphous diagram by means of bulk magnetization, anti .mu. (4.2/sup 0/K), Curie temperature, T/sub c/, and electrical resistivity, rho, measurements from 4.2/sup 0/K up to the amorphous-crystal transformation. The composition dependence of anti .mu. and T/sub c/ when B substitutes for P at c/sub Fe/ constant suggests the existence of two different short-range orders in the amorphous alloys, corresponding to the epsilon and epsilon/sub 1/ crystal structures in the Fe/sub 3/P/sub 1-x/B/sub x/ compounds. The concentration dependence of anti .mu. and T/sub c/ when P (or B) substitutes for Fe at c/sub B/ (or c/sub P/) constant is explained by a comparison between the amorphous Fe and the fcc Fe. A minimum in the variation of rho as a function of the temperature T occurs at T/sub m/. The temperature dependence of rho is expressed by a phenomenological law: rho(T) = rho/sub 0/ + A log T + B T/sup 2/ + CT. The concentration dependence of T/sub m/ and of the coefficients A and B is discussed in relation with the magnetic and structural properties of the amorphous Fe--P--B alloys. 10 figures, 1 table.

Concentration Dependence of the Magnetic Properties in Amorphous Fe-P-B Alloys

Concentration Dependence of the Magnetic Properties in Amorphous Fe-P-B Alloys
Author:
Publisher:
Total Pages:
Release: 1976
Genre:
ISBN:

The variation with composition of the magnetic properties of amorphous Fe--P--B alloys obtained by splat-cooling is discussed. For a given Fe concentration, the magnetic moment per atom anti .mu. and the Curie temperature T/sub c/ both increase with the substitution of B for P. The variation of anti .mu. and T/sub c/ as a function of the B content had the same discontinuity as that occurring between the two phases epsilon and psilon1 of the crystalline Fe3P/sub 1-x/B3 compounds. The variation of anti .mu. and T/sub c/ was also studied when one metalloid (P or B) substitutes for Fe, the other metalloid remaining constant. The value of anti .mu. was found to decrease when the P or B content is increased, as expected from a rigid band model. In the same concentration range, T/sub c/ increases with either P or B. The different behaviors of anti .mu. and T/sub c/ are tentatively explained by assuming that the amorphous Fe has two magnetic states (ferro and antiferromagnetic) as already suggested for crystalline Fe in a fcc environment.

Origin of Magnetic Properties in Amorphous Metals

Origin of Magnetic Properties in Amorphous Metals
Author: F. E. Luborsky
Publisher:
Total Pages: 60
Release: 1978
Genre:
ISBN:

The magnetic properties of amorphous metals are examined relative to changes in composition, processing, and heat treatment of amorphous transition metal-metalloid alloys. The transition metals examined were iron and iron plus nickel. These were alloyed with the metalloids boron, phosphorous, and carbon. Significant effects of alloy variation were observed on magnetic properties and on the crystallization and stress relief of these materials. Magnetic ageing was also observed and is interpreted in terms of a new mechanism. (Author).