By R. Troc, W. Suski (auth.), H.P.J. Wijn (eds.)
Volume 19 if team III bargains with the magnetic homes of metals, alloys and steel compounds. the quantity of knowledge to be had during this box isso vast 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 homes which count in simple 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 houses of actinide parts and their compounds. half 1 is anxious with the actinide components and their compounds with 3d, 4d and 5d-elements. the current half 2 includes info on compounds with major team components. A accomplished index of gear for volumes III/19a ... III/19f is incorporated. facts at the homes that rely on the instruction 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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Quantity 19 if workforce III bargains with the magnetic homes of metals, alloys and steel compounds. the quantity of data on hand during this box isso big 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 homes, i.
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Extra resources for Actinide Elements and their Compounds with other Elements. Part 2, 1st Edition
T plot for highpurity, well annealed, polycrystalline sample of U,,,,Th,,,,Be,, [91Kl]. AC(T,,) for this pure sample is more than twice as large as that reported by , y(O) = 2300 mJ mol-’ K-*. (b) T, vs. H plot for both transitions. The values of Bi2 (T,,) and II,* (T,,) are the sameand are equal to - 45(3)T K-r, as for pure UBe,,. 2 6 B IK b Fig. 55. U(Be,B),,. Specific heat data for polycrystalline UBe,2,9,B,,,,, . (a) C,/T vs. 2 K. The broken line indicates the AC, discontinuity at T, as expected from BCS theory.
Above T > 4 K, a T"' dependenceis observed. (b) shows the electronic spin fluctuation rate rNMRvs. log T. The temperature behaviour of this rate is different from that probed by neutrons (Fig. 67) [86Gl] and by Raman scattering (Fig. 70)[87C2]. The rNMRvalue is nearly two orders of magnitude smaller at low temperatures than that reported by neutron (Raman) measurements and it becomes consistent with the response expected from specific heat measurements. 72. UBe,,. gBe spin-lattice relaxation rate T;' for polycrystalline UBe,,, measured between 1 and 300 K [84C2], and 300 and 1000K [88Cl].
The solid line through the experimental points represents a fit to the theory discussed in the original paper, for which the dotted line is a particular limit. 8 T. C. There is no evidence of a second-phase behaviour, reported for a polycrystalline sample by [87Rl]. See also [SSSZ] and [89B2] for B,,(T) of pure, polycrystalline UBe,,. For this, but of UBe,, doped with different ions, see [91Dl] and references therein. LandoIl-B6mslcin New Series Ill/1912 Ref. p. 1 An-Be: figures 35 55 T/K 50 45 k ,” a?