Actinide Elements and their Compounds with other Elements. by R. Troc, W. Suski (auth.), H.P.J. Wijn (eds.)

By R. Troc, W. Suski (auth.), H.P.J. Wijn (eds.)

Volume 19 of team III (Crystal and sturdy nation Physics) bargains with the magnetic homes of metals, alloys and metal compounds. the quantity of data on hand during this box is so colossal that quantity III/19 needed to be break up into a number of subvolumes. Subvolumes III/19a via III/19f deal with the intrinsic magnetic houses, i.e. these houses which count basically at the chemical composition and the crystal constitution. to this point, subvolumes III/19a, III/19b, III/19c, III/19d2, III/19e1, and III/19e2 have seemed; III/19d1 will keep on with almost immediately. Subvolume III/19f covers the magnetic houses of actinide components 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 staff elements), that is due within the close to destiny, additionally encompasses a entire index of gear for volumes III/19a ... III/19f. facts at the homes that rely on the training of the samples measured, as for example, skinny movies, 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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Additional info for Actinide Elements and their Compounds with other Elements. Part 1

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42. 7-U. Energy band structure for bee uranium, calculated by the method indicated for Th (Fig. 38) with the exchange parameter a=2/3 and electron configuration (f3d’s2) [72 F 23. Trot, Suski [Ref. p. 85 Ref. p. 2 An: electronic Y 200 &&s cell Ry A r properties x CYHT E A ZAI-SOR Fig. 43. a-U. Energy band structure along the principal symmetry axes, calculated by self-consistent SRAPW method based on the local-density approximation [9OY I]. Only the part in the vicinity of the Fermi level, E,, is shown.

85 Fig. 45. u-U. Modified theoretical frequency branches (dashed lines, labelled by A, B, and C) and experimental ones (symbols and solid lines labelled by greek letters) of the dHvA effect as a function of the direction of the magnetic field in the three principal symmetry planes. The modification of the original FS is made by shifting E, of the 1 ith, 12th, 13th, and 14th bands such that the magnitude and the angular dependence fit to the experimental branches [8OS 11 as closely as possible [9OY 11.

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. 0at% U. The data indicate the formation of a nonmagnetic ground state (Kondo effect). Note a large shift of the temperature of the minimum with increasing U concentration. (b) Incremental rcsistivity AQ=Q-e,, vs. T’. The solid lines represent the equation shown in the figure with T,zlOOK [70M 11.

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