By R. Troc, W. Suski (auth.), H.P.J. Wijn (eds.)
Volume 19 if staff III offers with the magnetic homes of metals, alloys and steel compounds. the quantity of knowledge to be had during this box isso significant 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 count basically 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 parts and their compounds with 3d, 4d and 5d-elements. the current half 2 comprises details on compounds with major team parts. A accomplished index of gear for volumes III/19a ... III/19f is incorporated. facts at the homes that depend upon the education of the samples measured, as for example, skinny motion pictures, amorphous alloys or the magnetic alloys utilized in technical functions, 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
Composition x for polycrystalline U, -XTh,Be,3, at pressuresfrom 0 to 12 kbar [86Ll]. 29 b; Fig. 31. (U,Th)Be,,. Kubo-Toyabe (KT) zero-field @R relaxation rate crxr vs. 06 [90H2,90Hl]. 035with the Umoment of (10e3 ... lo-*)~a. 7K [91Hl]. 10’~ 8 lo-’ 2 L 6 B 1 2 L 6 K 10 I- Land&-BGmslcin New Series 111’1912 Ref. p. 5kOe(TF) . 2 - Fig. 32. UBe,,. 5 kOe [91Ll]. No change in gP+is seen at T,. This indicates that the penetration depth is very large (2 > 10000 A). The temperature-independent zerofield eP+gives proof of no magnetic order in UBe,, down to the lowest temperatures.
T of polycrystaliine UBe, 3 at eight pressurevalues ranging from 12 up to 152 kbar [90Ml]. Note a strong shifting of the p-maximum (T,,,,,) in the curves to peratures. 0 r-mm I IIRP.. 0 v I I I 100 @cm 150 I 125 QJ 100 10 25 100 150 200 250 0 K 300 b I I 20 40 60 80 P- 100 120 kbor 160 Ref. p. 1 An-Be: figures 120 kbar 160 0 c 20 kbor 160 Tmox - 60 80 K 100 Fig. 37. UBe,,. Effect of high pressure up to 152 kbar on the electrical resistivity of polycrystalline UBe,, [90Ml]. (a) Temperature of the resistivity maximum, Tmax,vs.
UBe,,. (a) Reciprocal magnetic molar susceptibility xi l of polycrystalline UBe,, vs. temperature [89B3]. 36 u&J, 0 = - 75 K. (b) shows x& ’ (in kOe/un units) at low temperatures. The dot-dashed curve represents the data of . 51 0 I 3 I 9 I 6 I 12 I 15 I K 18 T- Fig. 16. (U, Th)Be,,. 13 at low temperatures [84Sl]. [Ref. p. 1 An-Be: figures 30 Ii *lO. 0 % 35 Fig. 18. (U, M)Be,,. Superconducting transition temperature T,, molar magnetic susceptibility x,,, at 2 K, paramagnetic Curie temperature 0, and effective paramagnetic U moment pelf as a function of impurity doping concentration x of (a) La, (b) Y, (c) Lu, and (d) SC[87Z2].
Actinide Elements and their Compounds with other Elements. Part 2 by R. Troc, W. Suski (auth.), H.P.J. Wijn (eds.)