By H.P.J. Wijn, J.G. Booth, Y. Nakai, Y. Tsunoda
Volume 32 of crew III is a complement to quantity III/19 and offers with the magnetic houses of metals, alloys and metal compounds which comprise at the least one transition element.
The current subvolume III/32B presents accomplished and evaluated facts on magnetic houses of alloys and compounds of d-elements with major team components released generally within the earlier decade.
Read Online or Download Alloys and Compounds of d-Elements with Main Group Elements. Part 1 PDF
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Additional resources for Alloys and Compounds of d-Elements with Main Group Elements. Part 1
Inverse magnetic field at the temperatures indicated. Curves show results for (a) [Ref. p. 2 K. 794⋅104 G cm3 mol–1 [86B6]. See also [89G1]. Fig. 36. 14. Field-cooled (FC) and zero field-cooled (ZFC) magnetic susceptibilities and thermoremanent (TRM) magnetization as a function of temperature at low field (10 Oe) for a single domain single crystal [93T2]. Landolt-Börnstein New Series III/32B Ref. p. 10 3d elements with Cu 29 Fig. 38. 95. Magnetizations measured in terms of ln t at different temperatures (T < Tf = 29 K), rescale onto a unique master curve σ(T ln (t/τ 0)) for a given history of the sample: a field of 10 kOe is applied on a zero-field-cooled sample.
Full and dotted curves correspond to the wait times tw = 0 and 3000 s, respectively [87N3]. Landolt-Börnstein New Series III/32B 33 Fig. 47. 80. Temperature dependence of magnetization for T < 1 K. The best fit with a –B/T – CT2 law is displayed (1). After deduction of the nuclear contribution, the obtained T2 slope is in perfect agreement with the higher-T results (1 < T < 5 K) (2) [87M3]. See also [86A4, 86A5, 92B1]. Fig. 49. 99757. Magnetic viscosity S reaches a maximum value at the temperature Tm in applied magnetic field H, where S is defined by M = M0 + S ln (t/t0) with parameters M0 and t0.
Landolt-Börnstein New Series III/32B Ref. p. 10 3d elements with Cu Fig. 69. 9946. 05 Tf (a: experimentally observed asymmetry of the muon decay). The solid curve cor- 41 responds to the best fit by an inhomogeneous freezing model [86P2]. See also [85E1, 91K1]. Fig. 70. 95. Zero-field muon-spin-relaxation function Gz(t). Solid lines represent the best-fit curves. 4 K [85U2]. 10 3d elements with Cu Fig. 71. 95. Comparison of time correlation of Mn magnetic moment measured by neutron-spin Fig. 72.