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 no less than contain, the magnetic homes of a few designated teams of drugs. quantity 19 of staff III (Crystal and reliable kingdom Physics) bargains with the magnetic houses of metals, alloys and steel compounds containing no less than one transition aspect. the volume of data to be had has turn into so colossal that a number of subvolumes are had to hide all of it. the 1st subvolumes take care of the intrinsic magnetic houses, i. e. these magnetic homes which count simply at the chemical composition and the crystal constitution. info at the houses which additionally depend upon the coaching of the samples measured, as for example, skinny motion pictures or amorphous alloys and the magnetic alloys utilized in technical functions, could 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 parts. the second one subvolume, III/19 b (1987), covers the magnetic homes of the binary steel alloys and compounds of 3d transition parts with the weather of crew 1B, 2B and 3B of the Periodic method. the current subvolume III/19 c completes the survey of the magnetic info of the metal compounds of d transition-elements with components of the most teams of the Periodic approach of the weather. the most important 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 info for Alloys and Compounds of d-Elements with Main Group Elements. Part 2
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 . I7 I 700 800 1 L’ -1 I-. I [Ref. p. 71 I -51 900 1000K 1100 60 120 180 I- b 2LO K 300 Fig.
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 .
Fig. 5 [67Y I] pFeliab plane, forming ferromagnetic sheets 167Y I], cf. Fig. 19 at RT [78 C I] e”qQP (“Fe) Cmdsl e”qQ/2 (“‘Sn) ‘) 2, 3, “) ‘1 6, [mm/s] Relative to “Fe in iron. Relative to “‘Sn in BaSnO,, unless otherwise stated. Relative to ‘lgSn in white tin. Average hyperfine field. leq2Q/21. 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.