By R. Troc, W. Suski (auth.), H.P.J. Wijn (eds.)
Volume 19 of crew III (Crystal and stable kingdom Physics) offers with the magnetic houses of metals, alloys and metal compounds. the volume of knowledge on hand during this box is so vast that quantity III/19 needed to be break up into numerous subvolumes. Subvolumes III/19a via III/19f deal with the intrinsic magnetic houses, i.e. these houses which count merely at the chemical composition and the crystal constitution. up to now, subvolumes III/19a, III/19b, III/19c, III/19d2, III/19e1, and III/19e2 have seemed; III/19d1 will keep on with presently. Subvolume III/19f covers the magnetic homes of actinide parts and their compounds. the current half 1 is worried with the actinide components and their compounds with 3d, 4d and 5d-elements. half 2 (compounds with major team elements), that is due within the close to destiny, additionally features a finished index of drugs for volumes III/19a ... III/19f. facts at the houses that rely on the training of the samples measured, as for example, skinny motion pictures, amorphous alloys or the magnetic alloys utilized in technical functions, are compiled within the final subvolumes of III/19, viz. III/19g, III/19h and III/19i, of which III/19g and III/19h have already been published.
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Extra resources for Actinide Elements and their Compounds with other Elements. Part 1
Temperature at different applied magnetic fields. (b) shows pcf vs. H at 15K [85Nl]. 1 u&f. 2 An: magnetic 62 dhcp *“Cf 25 I I I 150 *ml 250 I [Ref. p. 85 properties /I 5 00 0 0 0 0 II 50 0 0 0 100 100 150 I- 200 250 K $0 Fig. 92. fee 24gCf. Reciprocal magnetic mass susceptibility xi ’ vs. temperature [76 F 23. 24 K. I- a 50 300 K 350 6 II? 5 1 I 0 b I 20 I 60 I 40 I 80 K 1O I- Fig. 91. dhcp 24gCf. (a) Reciprocal magnetic molar susceptibility 1, ’ vs. 6 u&f and Q=40K [85N 11, see also [87H 11. (b) shows the thermo-magnetization curve at 30 kOe, Tc= 51(2) K.
Both structures were determined by the self-consistent RLMTO method with an inclusion of both the spinpolarization and spin-orbit effects simultaneously [9OS2]. Note that in the case of 6-Pu the spectrum is anisotropic. For cr-Pu a nonmagnetic DOS, N(E), as well as the integrated DOS, N, are shown. For the spin and orbital magnetic moments in the framework of this approach, at given R,,, see Fig. 52. For a non-selfconsistent calculation of the spin moment only, for &Pu, see [87 S I]. Land&-Biimstein New Series III/l9fl Trek, Suski 48 [Ref.
For Fig. 54 see next page. II-. p-Am ? 6 I J. 1 Fig. 55. B-Am. Partial densities of occupied 5f states, NSf(E), broadened in order to compare with the UPS experiment of Am [84 N I]. Spectrum 1 is the LSD-only result, 2 is the SIC-LSD result for scheme I (5f7), and 3 is the SIC-LSD result for the scheme11 (5f6) [91 S I]. The dashed line is the photoemission valence spectrum. See also the caption to Fig. 54. 2 An: electronic properties [Ref. p. 85 N- O I K0 5 I I 25 50 a O 10 5 I 15 N(E) N10 15 -states cell I I 100 stotes cell RY l!