By R. Troc, W. Suski (auth.), H.P.J. Wijn (eds.)
Volume 19 if crew III offers with the magnetic homes of metals, alloys and steel compounds. the quantity of knowledge to be had during this box isso massive that quantity III/19 needed to be cut up into numerous subvolumes. Subvolumes III/19a via III/19f deal with the intrinsic magnetic homes, i.e. these homes which rely in simple terms at the chemical composition and the crystal constitution. to this point, subvolumes III/19a, III/19b, III/19c, III/19d, III/19e and III/19f1 have seemed. Subvolume III/19f covers the magnetic houses of actinide parts and their compounds. half 1 is worried with the actinide parts and their compounds with 3d, 4d and 5d-elements. the current half 2 comprises details on compounds with major workforce components. A accomplished index of gear for volumes III/19a ... III/19f is integrated. facts at the homes that rely on the instruction of the samples measured, as for example, skinny motion pictures, 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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Extra resources for Actinide Elements and their Compounds with other Elements. Part 2
F-derived specific heat, AC = CexpC,,, vs. log T [86Fl]. Cph is the lattice contribution determined from neutron inelastic scattering. The solid line is a Kondo contribution, the dashed line is a Schottky anomaly for doublet-quartet splitting (180 K). For experimental points and crystal-field analysis seethe original paper. These results are consistent with the ‘Be spin-lattice relaxation rate in UBe,, [88Cl] (seeFig. 72). 2 Fig. 58. UBe,,. CJT vs. T plot taken to the lowest temperature of 38 mK and at different magnetic fields (0 ...
Seealso [86Rl]. 01 0 I I 2 4 T- I I 6 8 K I 10 Fig. 24. UBe,,, (U, Y)Be,,. Left-hand side: Magnetoresistance R(H)/R(O) vs. 2 and 10 K for polycrystalline sample of (a) pure UBe,,, (b) U,,,,Y,,,,Be,, and (c) U,,,Y,,,Be,, [91A3]. The right-hand side shows the Kondo temperature TK as found by fitting the experimental data to the formula derived for the S = l/2 Coqblin-Schrieffer model [89Sl] at each measured temperature. Only for sufficiently diluted UBe,,, T, derived from the magnetoresistancebecomestemperatureindependent as is expected from the Kondo impurity system.
B) Same data as in (a), but plotted as log C, vs. log T. At the lowest temperatures C, (T) tends to vanish as p. For pure UBer, a T3 or T2,9 dependencewas reported, see  and [87R5], respectively. Land&Biimstein New Series III/19f2 [Ref. p. n. 05 0 3 %Fig. 56. (U, M)Be r 3. Electronic specific heat coefficient y(O) vs. 15 [90K2]. For smaller dopant atoms, such as SC, Y, Lu, Zr and Hf for which a, (MBe,,) < a, (UBe,,), y(O) per mol U is almost independent of concentration and amounts to 240% of that of pure UBe,,.
Actinide Elements and their Compounds with other Elements. Part 2 by R. Troc, W. Suski (auth.), H.P.J. Wijn (eds.)