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 workforce III (Crystal and good kingdom Physics) bargains with the magnetic homes of metals, alloys and metal compounds. the volume of data on hand during this box is so sizeable 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 rely merely at the chemical composition and the crystal constitution. thus far, 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 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 crew elements), that is due within the close to destiny, additionally incorporates a finished index of gear for volumes III/19a ... III/19f. info at the homes that rely on the guidance 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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Additional info for Actinide Elements and their Compounds with other Elements. Part 1

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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!

851 Fig. 47. a-U. Cross sections of the hole and electron sheets of FS in the llth, 13th and 14th bands (the 12th band is omitted because of too large an extremal area to be explained by the experiment) in l/8 of the Brillouin zone [90 Y 21. A and A’ show the small and large hole sheets, respectively, in the 11th band (see Fig. 46a). B shows the electron sheet in the 13th band (see Fig. 46~). C shows the electron sheet in the 14th band (see Fig. 46d). L 6' 03 I r A Hl- A Hl- E- Pu A Fig. 48. Comparison of the relativistic energy bands in the r-H(100) direction for -y-U, y-Np, and E-PU [74 F I].

C)Two equivalent, cylindrical, electron sheets of the FS in the 13th band, opened toward the [OOl] direction (branch B in Fig. 45). (d) Equivalent electron sheets of the FS in the 14th band loo11 (branch C in Fig. 45). 2 An: electronic properties Ref. p. 851 Fig. 47. a-U. Cross sections of the hole and electron sheets of FS in the llth, 13th and 14th bands (the 12th band is omitted because of too large an extremal area to be explained by the experiment) in l/8 of the Brillouin zone [90 Y 21. A and A’ show the small and large hole sheets, respectively, in the 11th band (see Fig.

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