By Y. Nakamura (auth.), H.P.J. Wijn (eds.)
Since 1970 a number of volumes of the Landolt-Börnstein New sequence have seemed that are dedicated to, or not less than contain, the magnetic houses of a few distinct teams of drugs. quantity 19 of workforce III (Crystal and stable country Physics) offers with the magnetic houses of metals, alloys and metal compounds containing not less than one transition point. the volume of knowledge on hand has develop into so massive that numerous subvolumes are had to hide all of it. the 1st subvolumes care for the intrinsic magnetic houses, i. e. these magnetic houses which rely purely at the chemical composition and the crystal constitution. info at the homes which additionally depend upon the coaching of the samples measured, as for example, skinny movies or amorphous alloys and the magnetic alloys utilized in technical purposes, should be compiled within the final subvolumes of the sequence. the 1st subvolume, III/19 a, seemed in 1986. It covers the magnetic houses of metals and alloys of the 3d, 4d and 5d transition components. the second one subvolume, III/19 b (1987), covers the magnetic houses of the binary metal alloys and compounds of 3d transition parts with the weather of team 1B, 2B and 3B of the Periodic method. the current subvolume III/19 c completes the survey of the magnetic facts of the metal compounds of d transition-elements with parts of the most teams of the Periodic method of the weather. the most important teams of ternary compounds, i. e. the Heusler alloys and the compounds with perovskite constitution, are being taken care of in separate chapters.
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Extra resources for Alloys and Compounds of d-Elements with Main Group Elements. Part 2
F&i. Fe-Si alloys at room temperature relative to the hypertine field in iron as a function of distance from the Si solute atom. The curve is drawn through the experimental points, which were obtained by the analysis of the Miissbauer spectra of 57Fe in Fe-Si alloys [66 S I]. are: lattice parameter of iron at room temperature. Land&-Biirnstein New Series IIIIl9c Nakamura [Ref. p. 5K 1 120It . ‘# 4 ,.. 12 16 kOe 20 . I 80 b 0 1, 8 HWrJl- Fig. 76. Fe,Si. Magnetization vs. 5 K [76 H 11. 0 Fig. 78.
Cm3 0 4 Ill0 5 10 15 20 ot% 25 Si - Fig. 74. F&i. Concentrations dependence of the electronic specific heat coefficient [64 G I]. --. liq 3, II Nl NT! a 0 2 4 Si - Fig. 71. Fe-Si. Paramagnetic Curie temperature 0, Curie constant C, and effective magnetic moment pea, of Fe-Si alloys in cl-phase and liquid state [68 P I]. 0 Shift of the hypertine field for s7Fe in Fig. 75. F&i. Fe-Si alloys at room temperature relative to the hypertine field in iron as a function of distance from the Si solute atom.
159. FeGe,. Schematicdiagram of the crystallographic structure. The valuesof spacingsd,, d2 and d, are given in Table 10,p. 46 [64 F I]. 100 300 200 l- K 400 Fig. 160. FeGe,. Temperature dependence of the magnetic susceptibility of a single crystal in magnetic fields parallel to the [OOI] and [llO] directions [71 M 11. 3 Alloys and compounds with Sn Survey Composition x Fe, -$nx FesSn Fe,%, Fe,Sn, Properties Figure x,- 1(xYT) x,- '(x2 T) p,(x), H,,,(x) at “Fe and p,(x), H,,,(x) at “Fe and p,(x), H,,,(x) at 57Fe and p,(x), H,,,(x) at 57Fe and crystal structure 161 162 P,,(H) P,,(T), f-XT) FeSn FeSn, “‘Sn ‘lgSn “‘Sn llgSn H,,,(T) at “Fe p,(x), H,,,,$x) at “Fe and “‘Sn xgm x, 07 magnetic structure H,,,(T)/H,,,(20 K) at “Fe and “‘Sn(1) p,(x), Hhyp(x)at 57Fe and ‘lgSn x, ‘VI o(T), fflc, UC H,,,(T) at “‘Sn Nakamura Table 163, 164 164 164 164 165 166 167 168 164 11 11 11 11 169 170 171 164 172 173 174 11 Ref.