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

Volume 19 if workforce III bargains with the magnetic houses of metals, alloys and steel compounds. the quantity of data on hand during this box isso massive 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 homes, i.e. these houses which rely in basic terms at the chemical composition and the crystal constitution. thus far, subvolumes III/19a, III/19b, III/19c, III/19d, III/19e and III/19f1 have seemed. Subvolume III/19f covers the magnetic homes of actinide components and their compounds. half 1 is anxious with the actinide parts and their compounds with 3d, 4d and 5d-elements. the current half 2 includes details on compounds with major crew parts. A complete index of gear for volumes III/19a ... III/19f is integrated. info at the houses that rely on the training of the samples measured, as for example, skinny movies, amorphous alloys or the magnetic alloys utilized in technical purposes, of III/19, viz. III/19g, III/19h and III/19i, of which III/19g, III/19h and III/19i2 have already been published.

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Additional resources for Actinide Elements and their Compounds with other Elements. Part 2

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Temperature dependence of longitudinal (q) and transverse (cr) elastic constants for polycrystalline UBe,, [SSYl]. The bulk modulus at 200 K, B. = 161GPa. Landoh-BCmslcin New Series lW19r2 Ref. p. 1 An-Be: figures 29 4 Fig. 13. UBe,,. Reciprocal magnetic molar susceptibility xi l of polycrystalline UBe,, vs. 4 u&J between 260 and 1100K) [71Tl]. 1000 mol a I300 I 600 ‘2 400 200 P I LOO I 200 0 I 600 T- 800 1000 K 1200 6 -zl~ cm3 250 0 200 150 I ‘G 5 IO 15 /hH - 20 T 25 Fig. 15. UBe,,. Magnetization r~ of polycrystalline UBe,, at low temperatures and magnetic fields up to 24 T [86Rl].

A) Thermal conductivity K between 5 and 14 K and (b) derivative dK/dT between 4 and 17 K for the single-crystalline sample of UBe,, [91Al]. 5 K. This probably is causedby a change in the degeneracyof the 5f crystal field ground state which results in a strong growth of C,, below 8 K [91Al]. 1 An-Be: figures Ref. p. 0 b Fig. 45. UBe,,. (a) Low-temperature thermal conductivity K for polycrystalline UBe,, [87R5]. (b) shows K vs. T up to 1 K. c. I I I. 0 . ’ I I II I4K . 102 T/Tm,x - Fig. 46. Hall coefficient R, as a function of temperature.

B) shows Q(T) for both U-based compounds at low temperatures. e. at the sametemperature at which a steep rise,in C/T (seeFig. 48a) and p(r) (seeFig. 19)setsin. 7 K, Q(r) of UBe, a reachesa value of - 13 uV K - ‘. For the Th-doped sample,Q(7’) goes through a broad negative minimum near 15 K. Land&Biimstein New Series III/1912 [Ref. p. 1 An-Be: figures 42 I 8 6 E < 3 170 4 pRcm 2 ; :: 160 2 20 -2 -8o8 6 810 ‘ 22 sal0' sal0’ 22 75 K 90 T- 110 Fig. 43. Thermal conductivity K, its electron part K,, electrical resistivity p, and Seebeck coefficient Q as a function of temperature for UBe,, single crystal [91Al].

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