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Superzone boundaries

The resistivities of the magnetic borides DyB, H0B12, ErB, and TmB, have been carefully measured by Gabani et al. (1999) for good quality crystals with low room temperature resistivities (10-30 p 2 cm) compared to the early work. Near the antiferromagnetic transition temperatures Tn, the resistivities all show small increases in the form of humps and then rapid drops as the temperature is lowered. This behavior can be explained as an initial increase in the resistivity attributed to the appearance of superzone boundaries within the Brillouin zone, followed by a decrease due to a reduction in spin scattering (Taylor and Darby, 1972 Fournier and Gratz, 1993). [Pg.113]

Fig. 14.36. Schematic repiesentation of the evaluation of the spin disorder resistivity (a) Usual extrapolation scheme valid from temperatures above the Debye temperature, (b) The case of dysprosium which has an antiferromagnetic temperature range where superzone boundaries raise the resistivity, (c) The case of an antiferromagnet which does not become ferromagnetic at low temperatures Superzone boundaries may distort results in the whole ordered range (Gratz and Poldy, 1977). Fig. 14.36. Schematic repiesentation of the evaluation of the spin disorder resistivity (a) Usual extrapolation scheme valid from temperatures above the Debye temperature, (b) The case of dysprosium which has an antiferromagnetic temperature range where superzone boundaries raise the resistivity, (c) The case of an antiferromagnet which does not become ferromagnetic at low temperatures Superzone boundaries may distort results in the whole ordered range (Gratz and Poldy, 1977).
Electrical resistivity measurements on single crystals in the [001] direction by Stalinski et al. (1973) showed that the spin disorder resistivity of RSns compounds was not proportional to the de Gennes factor. Since these materials are antiferromagnetic superzone boundary effects might render impossible the estimation of the spin disorder resistivity as described in subsection 2.1. On the other hand, since the shape of the dp/dT curve of NdSns around the N6el temperature was qualitatively similar to that expected by the theory of... [Pg.116]

De Gennes and Saint James (1963) explained the temperature variation of the spin periodicity in the HAFM structure near by the effects of conduction electrons scattering by the 4f spin disorder. EUiott and Wedgewood (1964) considered the influence of superzone boundaries introduced by the helical structure into the energy spectrum of the conduction free electrons. They showed that with an increase of the 4f spin order the value of Q should decrease and the first-order HAFM-FM transition should occur. Miwa (1965) in his model took into account both these factors. On the base of Miwa s model Umebayashi et al. (1968) obtained the following ejqiression for the pressure dependence of (p... [Pg.117]


See other pages where Superzone boundaries is mentioned: [Pg.152]    [Pg.156]    [Pg.161]    [Pg.162]    [Pg.424]    [Pg.503]    [Pg.583]    [Pg.741]    [Pg.351]    [Pg.66]    [Pg.96]    [Pg.491]    [Pg.497]    [Pg.152]    [Pg.156]    [Pg.161]    [Pg.162]    [Pg.424]    [Pg.503]    [Pg.583]    [Pg.741]    [Pg.351]    [Pg.66]    [Pg.96]    [Pg.491]    [Pg.497]    [Pg.474]   
See also in sourсe #XX -- [ Pg.66 , Pg.96 ]




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Superzones

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