Parametrization of transition-metal Fermi-surface data

1975 ◽  
Vol 11 (4) ◽  
pp. 1447-1459 ◽  
Author(s):  
J. B. Ketterson ◽  
D. D. Koelling ◽  
J. C. Shaw ◽  
L. R. Windmiller
2019 ◽  
Vol 36 (5) ◽  
pp. 057402 ◽  
Author(s):  
Xi Zhang ◽  
Tianchuang Luo ◽  
Xiyao Hu ◽  
Jing Guo ◽  
Gongchang Lin ◽  
...  

1991 ◽  
Vol 231 ◽  
Author(s):  
J. Mathon

AbstractA general theory of oscillations in the exchange coupling between two transition metal ferromagnets separated by a nonmagnetic transition metal spacer is developed. A close analogy between oscillations in the exchange coupling and de Haas-van Alphen oscillations is established and exploited to show that the period, asymptotic decay, and temperature dependence of the oscillations are determined by properties of the d band Fermi surface in the spacer layer. The theory accounts qualitatively and even semiquantitatively for all the salient experimental features of the oscillations in the exchange coupling observed recently in Co/Ru, Co/Cr, and Fe/Cr superlattices.


2009 ◽  
Vol 6 (S6) ◽  
pp. 395-402 ◽  
Author(s):  
Jerry C. Shaw ◽  
J. B. Ketterson ◽  
L. R. Windmiller

2017 ◽  
Vol 694 ◽  
pp. 439-451 ◽  
Author(s):  
Masashi Kakihana ◽  
Hiromu Akamine ◽  
Keisuke Tomori ◽  
Kengo Nishimura ◽  
Atsushi Teruya ◽  
...  

1971 ◽  
Vol 49 (19) ◽  
pp. 2449-2461 ◽  
Author(s):  
P. T. Coleridge ◽  
I. M. Templeton

The Fermi surface neck size and the scattering cross sections for the neck and [Formula: see text] belly orbits have been measured in dilute alloys of Zn, Al, Ge, Si, Ni, Co, Fe, Mn, and Cr in Cu. Earlier observations of rigid-band behavior for the neck size in Cu(Zn) and Cu(Al), while essentially substantiated by the present measurements, are now believed to be fortuitous; Cu(Ge) and Cu(Si) do not agree with a rigid-band prediction. The changes (generally reductions) of neck size in the transition metal alloys do not appear to be related directly to changes of electron concentration. The scattering anisotropy is rather small in the heterovalent alloys, the scattering being somewhat greater on the necks, but is large and in the opposite sense in the transition metal alloys. The magnitude and anisotropy of scattering is interpreted in terms of phase shifts associated with the impurities and the wave functions over the Fermi surface. There is evidence for additional scattering anisotropy in alloys exhibiting the Kondo effect.


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