By R. Troc, W. Suski (auth.), H.P.J. Wijn (eds.)
Volume 19 of staff III (Crystal and reliable kingdom Physics) offers with the magnetic houses of metals, alloys and metal compounds. the quantity of data on hand during this box is so great 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 houses, i.e. these homes which count in simple terms 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 stick to presently. Subvolume III/19f covers the magnetic houses of actinide parts and their compounds. the current half 1 is worried with the actinide parts and their compounds with 3d, 4d and 5d-elements. half 2 (compounds with major crew elements), that is due within the close to destiny, additionally encompasses a finished index of drugs for volumes III/19a ... III/19f. information at the houses that depend upon the training 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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Quantity 19 of team III (Crystal and strong country Physics) offers with the magnetic houses of metals, alloys and steel compounds. the quantity of data to be had during this box is so giant 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.
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Additional resources for Actinide Elements and their Compounds with other Elements. Part 1, 1st Edition
26 N&)/(1 + N(E,)) [88 S 11. Olb I I I Th PO u NP Pu Fig. 57. Light An. Bulk properties of light actinide metals calculated by means of the LMTO method within ASA and with so-called combined correction terms [90 S 31 for the fee crystal structure. (a)Comparison of calculated values for the atomic volume using different levels of approximations with experimental ones [74 D 11. (b)Comparison of calculated values for the linear coefficient of thermal expansion E with experimental ones [64 G I], for U [63 B I].
3 Rv IX Fig. 44. u-U. (a) Total and partial density of states as a function of energy [9OY I]. 7 states/Ry and cell) at E,. 14 mJ Km2 mol-’ [75 B 23). (b) Theoretical result for the DOS of the 5f bands (solid line) as a function of energy [9OY I], compared with the experimental XPSBIS spectrum [80 B 21, shown by dashed line. 2 An: electronic properties 44 ! a- u I, El \, / I “ho/ . A: i / I7 A (001) (010) I I 0" L5" 90" 45" [OlOl Field angle 0” I1001 45” [Ref. p. 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.
85 properties 20 s fee Np -6 -4 -2 0 2 4 6 8 ev 10 E- Fig. 49. Np. Total density of states, N(E), of neptunium in the phases (a) hypothetical fee, (b) bee (y-phase) and (c) tetragonal P-phase, determined in self-consistent, fully relativistic, LMTO (linear muffin-tin orbital) calculations [88 B 11. 5eV) are due to 6d electrons. The results show decreasing 6d-5f hybridization on going from the P-phase to the fee phase (narrowing of the DOS functions). Trot, Suski Ref. p. 2 An: electronic properties I 50 N(E)- r 47 I 100 I states 200 cell Ry X Fig.