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 a minimum of comprise, the magnetic homes of a few specified teams of gear. quantity 19 of workforce III (Crystal and stable kingdom Physics) bargains with the magnetic homes of metals, alloys and steel compounds containing no less than one transition aspect. the quantity of knowledge on hand has develop into so massive that numerous subvolumes are had to disguise all of it. the 1st subvolumes care for the intrinsic magnetic houses, i. e. these magnetic homes which rely basically at the chemical composition and the crystal constitution. information at the homes which additionally rely on the practise of the samples measured, as for example, skinny motion pictures 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 homes 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 components with the weather of workforce 1B, 2B and 3B of the Periodic method. the current subvolume III/19 c completes the survey of the magnetic info of the steel 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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Additional info for Alloys and Compounds of d-Elements with Main Group Elements. Part 2
E”qQ(1 + q2/3)l12/2. 876) at IIOK [Ref. p. 3 Fe-Sn 1050 1150 1250 l- 1350 Fig 161. Fe&n. 82at% Sn [65A I]. 1450 K 1550 1350 lFig. 162. Fe-Sn. 14at% Sn. [65A I]. 30 /’ /’ JJ 1. 20 0 Fe 1 2 3 4 Sn- 5 6 7 or/o8 Fig. 163. Fe-Sn. Saturation magneticmomentat 77 K vs. composition [70T I]. Ood__ll__loo Fe 0 Sn- Sn Fig. 164. Fe-Sn. Saturation magneticmoments(solid circles) and magnetic hyperhne fields for 57Fe (open circles) and iL9Sn (triangles) at 77K [70T I]. 3 Fe-Sn Ref. p. 4 0 Thermal variation of the Fe magneFig.
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].
112. Fe, -,Cr,Si. Magnetic susceptibility vs. temperature (a) and composition at T= 80 K (b) [69 S I]. Land&-Biirnstein New Series III/l9c. 1 Fe-C, Si [Ref. p. 71 160 x-6 cm3 -is120 I I/ - 0 I I 10 20 30 40 1 2 3 4 I I I J 50 kOe 60 a 0 70 110 150 190 230 270 K 310 a 1 150 k 100 50 0 . 8 *lo3g/cm3 6 b Hopp~ IO‘- Fig. 114. Fe, -,Mn,Si. [84 N 11. 0 Fig. 113. 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.
Alloys and Compounds of d-Elements with Main Group Elements. Part 2 by Y. Nakamura (auth.), H.P.J. Wijn (eds.)