By R. Troc, W. Suski (auth.), H.P.J. Wijn (eds.)
Volume 19 of staff III (Crystal and sturdy country Physics) bargains with the magnetic homes of metals, alloys and metal compounds. the quantity of data to be had during this box is so vast that quantity III/19 needed to be cut up into a number of subvolumes. Subvolumes III/19a via III/19f deal with the intrinsic magnetic homes, i.e. these homes which rely purely at the chemical composition and the crystal constitution. to date, subvolumes III/19a, III/19b, III/19c, III/19d2, III/19e1, and III/19e2 have seemed; III/19d1 will stick with almost immediately. Subvolume III/19f covers the magnetic houses of actinide components and their compounds. the current half 1 is anxious with the actinide components and their compounds with 3d, 4d and 5d-elements. half 2 (compounds with major workforce elements), that's due within the close to destiny, additionally encompasses a complete index of drugs for volumes III/19a ... III/19f. info at the homes that rely on the practise of the samples measured, as for example, skinny motion pictures, amorphous alloys or the magnetic alloys utilized in technical purposes, 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 info for Actinide Elements and their Compounds with other Elements. Part 1
Temperature at the atmospheric pressure and at 2 GPa. between 700 and 1300K [89 S 21. (b) shows the room-temperature resistivity up to IOGPa, and (c) the temperature coefficient of the resistivity (6~/6T)/~(300K) as a function of temperature at atmospheric pressure and at 2 GPa. 2 An: electrical properties 64 [Ref. p. 85 Fig. 97. Th. 2K [59B 11, e(T)=@ (B = 0, T). 2 for Th 1 and Th 2, respectively. The dashed line represents data by [29 K 11. 67 T- Fig. 98. Th(U) alloys. (a) Electrical resistivity e vs.
6 eV energies [84N I]. 8 eV excitation energy of Am and Pu [82 that of Sm (unpublished). Land&-BBmstein New Series III/19fl Trot, Suski spectra of excitation spectra at N l] with [Ref. p. 36 0 50 100 I- Fig. 64. Light An. Summary picture of magnetic molar susceptibility x,, vs. temperature for the light actinide metals. 150 I- 200 250 300 K 3 Fig. 65. Th. Specific magnetic susceptibility xs of highmetal vs. 2 K) z 1300. 04 Gcm3 9 0 20 40 60 80 kOe 3 H- I- Fig. 66. Th(U) alloys. (a) Specific magnetic susceptibility xp of pure Th and dilute Th(U) alloys vs.
Land&Bhstein New Series III/i9fl 200 T- a 20 40 60 80 K 100 T- Fig. 79. (a, b) Differential magnetic susceptibility Axg (from torque data) in three principal planes as a function of temperature [7OA 21. Trot, Suski I [Ref. p. 2 An: magnetic properties 58 mo! 10 in? 05 I 250 300 Fig. 80. &Pu. Molar magnetic susceptibility xrn vs. temperature for (a) &Pu(Ga) and (b) &Pu(AI) alloys [67 L 31. 350 650 750 K TO Fig. 81. Pu. Specific magnetic susceptibility lB at high temperatures [61 S 11. See also [90 S 11.