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

ISBN-10: 3540467297

ISBN-13: 9783540467298

ISBN-10: 354055114X

ISBN-13: 9783540551140

Volume 19 if team III bargains with the magnetic homes of metals, alloys and metal compounds. the volume of knowledge on hand during this box isso immense 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.e. these homes which count purely 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 components and their compounds. half 1 is worried with the actinide components and their compounds with 3d, 4d and 5d-elements. the current half 2 includes info on compounds with major crew components. A complete index of gear for volumes III/19a ... III/19f is integrated. facts at the houses that depend upon the training 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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Additional info for Actinide Elements and their Compounds with other Elements. Part 2

Sample text

If superconductivity would not occur in UBe,,, the magnetic ordering at x 150 mK and H = 0 could be apparent. Compare these data with those given by [86Ml] and [87F3]. Landoh-FGmstcin New Series 111’19f2 Ref. p. 2 2 4 6 8 10 K 20 T- Fig. 59. UBe,,. Pressure dependence of C,/T for polycrystalline UBe,, [87Pl]. Pressure values are indicated in the figure. e20 K is given in logarithmic scale. 5 K of the p vs. 23 K/kbar, as in the electrical resistivity vs. pressure experiment [87T2] (cf. Fig. 35a).

At the lowest temperatures C, (T) tends to vanish as p. For pure UBer, a T3 or T2,9 dependencewas reported, see [8702] 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,,. , with the distance du-ac. 1 limit (nonconcentrated regime).

25 0 50 100 150 200 250 K 300 1 1 10 a 10' lo3 K 1 I- Fig. 71. UBe,, (a) ‘Be nuclear spin relaxation rate T;' vs. T for polycrystalline UBe, 3 [88B2]. 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.

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Actinide Elements and their Compounds with other Elements. Part 2 by R. Troc, W. Suski (auth.), H.P.J. Wijn (eds.)


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