3d, 4d and 5d Elements, Alloys and Compounds by H. P. J. Wijn (auth.), H. P. J. Wijn (eds.)

By H. P. J. Wijn (auth.), H. P. J. Wijn (eds.)

Volume 32 of team III is a complement to quantity III/19 and should take care of the magnetic houses of metals, alloys and metal compounds which include at the very least one transition element.
The current subvolume III/32A presents finished and evaluated information on magnetic houses of 3d, 4d and 5d parts, alloys and compounds released in general within the earlier decade.

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7. 99 wt% pure, annealed at 360 “C for 168 h. Lattice parameter a determined from the (600)-diffraction line of a MO target and c determined from the (400)-reflection of an Fe target. 10e5below 50 K. The ratio c/u obtained by using the X-ray Bond’s method [8801, 89021. 15 600 570 565 615 600 I- 630 * 645 K 660 Fig. 8. 999 wt%. Magnetic contribution a,,, to the linear thermal expansion coefficient measured by a neutron back-scattering technique as a function of temperature T. Error bar indicated.

17, it is ascribed to long range magnetic order as a result of reverse polarisation of the 4s conduction band [92Bl]. 45 ~1~with Tc well above RT [92B2]. Results of linear momentum distributions of the unpaired-spin electrons, the so-called magnetic Compton profiles, of Fe, Co and Ni as measuredwith various techniques are reproduced in the Figs. 18-22. For ab-initio calculations in the case of Ni see [88SlJ. For the local magnetic moments of 3d, 4d and 5d transition metal inpurities in Fe and Ni see the Figs.

Phys. Sot. Jpn. : J. Magn. Magn. Mater. : J. Phys. : J. Phys. Sot. Jpn. : J. Phys. : J. Phys. : Solid StateCommun. : J. Phys. : Phys. Rev. : Fiz. Met. Metalloved. 48 (1979) 1158; Phys. Met. Metallogr. (Engl. : J. Phys. : J. Magn. Magn. Mater. : J. Phys. Sot. Jpn. : J. Phys. : J. Appl. Phys. : J. Phys. Sot. Jpn. : J. Phys. : J. Phys. : J. Magn. Magn. Mater. : J. Magn. Magn. Mater. : Phys. Rev. Lett. : J. Magn. Magn. Mater. : J. Phys. : Phys. Rev. : Solid StateCommun. : J. Phys. : Phys. Rev. : J.

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