Alloys and Compounds of d-Elements with Main Group Elements. by H.P.J. Wijn, J.G. Booth, Y. Nakai, Y. Tsunoda

By H.P.J. Wijn, J.G. Booth, Y. Nakai, Y. Tsunoda

Volume 32 of workforce III is a complement to quantity III/19 and offers with the magnetic homes of metals, alloys and steel compounds which comprise at the very least one transition element.
The current subvolume III/32B presents complete and evaluated facts on magnetic homes of alloys and compounds of d-elements with major staff components released quite often within the prior decade.

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Extra resources for Alloys and Compounds of d-Elements with Main Group Elements. Part 1

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Landolt-Börnstein New Series III/32B Ref. p. 10 3d elements with Cu 61 Ni− −Cu Ni and Cu form a continuous series of solid solutions [90m1]. Numerous experimental data were published before 1984 and are compiled in Landolt-Börnstein, vol. III/19A edited by G. Zibold. 476. In the last decade, ternary alloy systems are mainly studied. Table 9. Ni–Cu–X. Freezing temperature Tf and Curie temperature TC. h and q mean homogenized and quenched samples, respectively. 1 29 Pd 7 21 93 50 Landolt-Börnstein New Series III/32B X [at%] Tf [K] TC [K] Ref.

104). Table 8. 99–yAuy. Magnetic parameters obtained by ac susceptibility and Mössbauer data. Hhf and ΓH denote average hyperfine field and the width of hyperfine field distribution, respectively [88F3]. 10 3d elements with Cu [Ref. p. 105 Fig. 101. Mn–Cu–Au. Magnetic contribution to the electrical resistivity vs. temperature [89S1]. 4⋅10−5 at% Fe at room temperature. The stable state at low temperature is an FeCu alloy with Fe precipitates. Magnetism of precipitates is beyond the scoop of the present subsection.

105 Fig. 56. 97. Absolute value of NMR enhancement factor η and NMR spin lattice relaxation rate T1–1 as a function of a small applied field H0. H0 was sweeped from zero to negative fields and then back to zero field. 76 kOe [88J1]. Fig. 58. 97. 76 kOe [91T1]. Landolt-Börnstein New Series III/32B Ref. p. 10 3d elements with Cu Fig. 59. MnxCu1–x. Temperature dependence of mean hyperfine field observed by PAC [84R3]. 37 Fig. 60. Mn–Cu. 1 and 10 at% Mn [85T1]. Fig. 61. 92. Kinetics of decay of ESR signal intensity in cooling in a magnetic field of 8 kOe.

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