Actinide Elements and their Compounds with other Elements. - download pdf or read online

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 workforce III bargains with the magnetic houses of metals, alloys and steel compounds. the volume of data to be had during this box isso vast 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 rely purely 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 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 includes details on compounds with major team components. A entire index of drugs for volumes III/19a ... III/19f is incorporated. facts at the houses that rely on the guidance 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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Extra resources for Actinide Elements and their Compounds with other Elements. Part 2

Example text

Reduced temperature T/T, (solid line) compared to experimental data of two heavy-fermion systems: UBe,, (closed circles) [8404] and CeCu,Si, (open circles) [83Bl]. Tf = 8 K. A two-component model was applied which requires both heavy (yr) and light (ya) electrons as well as their interactions. Thus C(T) is given by the equation, C(T) = y,T{ 1 + 7c2T2/3 [7/5&'/p, - (p;/p#]}, where pr is the DOS of the fcomponent taken as Lorentzian. For details see original paper [87Fl]. 5 0 a 100 200 T- 300 400 0 K 500 b 2 4 6 8 10 K 12 T- Fig.

12. 2 and 80 K [85G3]. The velocity passesthrough several anomalies; a maximum at 25 K, a minimum around 2 K (corresponding to the temperature of specific heat and electrical resistivity maxima) and a small jump at 1 K due to the superconducting transition. 0 o. 5I 0 25 50 15 100 125 K 150 Fig. 11. UBe,,. 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.

11. UBe,,. 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,,.

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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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