Download Alloys and Compounds of d-Elements with Main Group Elements. by Y. Nakamura (auth.), H.P.J. Wijn (eds.) PDF

By Y. Nakamura (auth.), H.P.J. Wijn (eds.)

Since 1970 numerous volumes of the Landolt-Börnstein New sequence have seemed that are dedicated to, or at the least comprise, the magnetic homes of a few detailed teams of drugs. quantity 19 of team III (Crystal and strong country Physics) offers with the magnetic homes of metals, alloys and metal compounds containing no less than one transition point. the quantity of data to be had has turn into so great that numerous subvolumes are had to conceal all of it. the 1st subvolumes take care of the intrinsic magnetic houses, i. e. these magnetic houses which rely in simple terms at the chemical composition and the crystal constitution. information at the houses which additionally rely on the guidance of the samples measured, as for example, skinny motion pictures or amorphous alloys and the magnetic alloys utilized in technical purposes, might be compiled within the final subvolumes of the sequence. the 1st subvolume, III/19 a, seemed in 1986. It covers the magnetic homes of metals and alloys of the 3d, 4d and 5d transition components. the second one subvolume, III/19 b (1987), covers the magnetic homes of the binary metal alloys and compounds of 3d transition components with the weather of team 1B, 2B and 3B of the Periodic process. the current subvolume III/19 c completes the survey of the magnetic information of the steel compounds of d transition-elements with parts of the most teams of the Periodic procedure of the weather. the main teams of ternary compounds, i. e. the Heusler alloys and the compounds with perovskite constitution, are being handled in separate chapters.

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Additional resources for Alloys and Compounds of d-Elements with Main Group Elements. Part 2

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Fig. 171. FeSn. Mean value of the reduced magnetic hyperfine fields for 57Fe and l*gSn(l) as functions of reduced temperature. The Brillouin curve for S = 1 is also included [75 H 11. 5 1 -$? 5 0 t 1 b 150 300 450 600 K 750 Fig. 172. FeSn,. Inverse magnetic susceptibility temperature curve [60 K 11. vs. -5 I1 0 0 40 80 120 160 K 200 Fig. 173. FeSn,. 3 kOe parallel and perpendicular to the tetragonal c axis of a single crystal. The dashed line indicates the transition from a noncollinear magnetic structure at low temperatures to a collinear antiferromagnetic structure at higher temperatures [85 V 11.

Fe, -,Co,Si. Tempcratorc dcpcndencc of the magnetization at 8 kOe and the reciprocal of the magnetic susceptibility [72S 11. Fig. 120. Fe, -,Co,Si. 2 K [79 B 11. Nakamura Magnetization vs. magnetic Landoh-B6mslein New Series 111’19~ Ref. p. 0 CoSi Fig. 121. Fe, -,Co,Si. Saturation magnetic moment per Fe atom at OK in the ferromagnetic phase, effective paramagnetic moment and paramagnetic Curie temperature vs. Co content [72 S I]. I -I;-’ Fe,-,CoxSi Lg I FeSi Fig. 122. Fe, -,Co,Si. 2 K as a function Co content, as estimated from the satellite of the magnetic peak measured by neutron small-angle scattering [83 B I].

Fe, -,Mn,Si. Magnetic susceptibility vs. temperature(a) and composition at T=80K (b) [69 S I]. 1 Fe-C, Si Ref. p. 0 MnSi Fig. 115. Fe, -,Mn,Si. Mn concentration dependence of the paramagnetic Curie temperature and the effective magnetic moments per Mn atom and per 3d atom 0 5 10 20 Fig. 116. Fe,-,Mn,Si. Temperature the hyperfine field at 57Fe [84N I]. [69Sl]. 00 MnSi Fig. 117. Fe, -,Mn,Si. (a) Magnetic phase diagram (Happt vs. 2K and (b) Curie temperature vs. Mn concentration [84N I]. 1 Fe-C, Si a L 100 200 I- 300 1-1 400 500 I I- 600 .

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