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 stable country Physics) bargains with the magnetic houses of metals, alloys and steel compounds. the volume of knowledge 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.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 persist with presently. Subvolume III/19f covers the magnetic homes of actinide parts and their compounds. the current half 1 is anxious with the actinide parts 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 features a entire index of gear for volumes III/19a ... III/19f. info at the homes that depend upon 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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Additional resources for Actinide Elements and their Compounds with other Elements. Part 1

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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. Fig. 46. a-U. Various hole and electron sheets of FS made from four bands, llth-14th, with a strong 5f character [90 Y 11. (a) Hole sheets of the FS in the 11th band which consists of the closed sheet centered at the T point (not observed branch) and two small ellipsoidal sheets whose principal axis points to the [OlO] direction (branch A in Fig.

P. 851 I fee Am (f6d1s2: \ u=lWMT r A xzw 0 Fig. 53. S-Am. Energy band structure of fee Am, calculated by the method indicated for Th (Fig. 38) using the full Slater exchange parameter (cr=l) with a (f6d’s2) L h I- c configuration. The results are similar to those of fee Cm [72 F 21. For the relativistic energy band structures of Am, Cm, and Bk with CI= 2/3 see [74 F I]. 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].

I=& -377 -375 ev-373 Fig. 59. Th, U. XPS core levels 4f,,,. Note a satellite below the main 4f,,, line for thorium metal ascribed to the screening (shake-up process) of the 5f’ state. No such a satellite can be found in XPS for uranium metal though the satellite exists (see Fig. 60) [74 F 23 and [SO B 11. I -12 ! I -8 -6 \ eV 0 f-fi-----, f-f, Fig. 60. a-U. Resonant photoemission spectra of polycrystalline a-uranium in the region of the 5d-5f Fanotype resonance (90eV~hv~108eV) [Sl 11-J. 3eV below E, is attributed to a more localized final 5f” state (n = 1 or 2) according to the prediction of [8OJ 11.

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