By R. Troc, W. Suski (auth.), H.P.J. Wijn (eds.)
Volume 19 of workforce III (Crystal and sturdy kingdom Physics) bargains with the magnetic houses of metals, alloys and steel compounds. the volume of data to be had during this box is so big 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 houses which count 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 to almost immediately. Subvolume III/19f covers the magnetic houses of actinide parts 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 staff elements), that's due within the close to destiny, additionally incorporates a complete index of drugs for volumes III/19a ... III/19f. info at the houses that rely on the guidance of the samples measured, as for example, skinny movies, 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 resources for Actinide Elements and their Compounds with other Elements. Part 1
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! , ru b L r X W KO 145 l(E) - Fig.
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. temperature. (b) Magnetic molar susceptibility excess, Ax,, due to the uranium impurities vs. temperature. 43u,/U and Q= -309K [70M 11. Fig. 67. Th. Magnetization c vs. applied magnetic tield H at 2K [71 F 11. Trot, Suski Iandolt-Biknstein New Series 111,‘19fl Ref. p. 2 An: magnetic properties 55 I I 0 50 100 , 150 T- 200 250 300 K 350 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. Similar conclusions are drawn from EELS (electron energy loss spectroscopy) [84 M 1-J. - Fig. 61. a-U. Combined XPS-BIS spectrum [80 B 23. Trot, Suski Landolf-BBmstein New Series 111~19fI Ref. p. 1 PU~PIW~ PU5s I I I -1400 -1200 -1000 I I -800 -600 E-E, - I -400 Pu 6s, 6p L -200 ev 0 Fig.
Actinide Elements and their Compounds with other Elements. Part 1 by R. Troc, W. Suski (auth.), H.P.J. Wijn (eds.)