2002
DOI: 10.1088/0953-8984/14/4/315
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Itinerant ferromagnetism of systems with double orbital degeneracy

Abstract: In this paper we study the ground state ferromagnetism in a doubly orbitally degenerate Hubbard model generalized by taking into account correlated hopping and inter-atomic exchange interaction. We find that an important role in the stabilization of ferromagnetism is played by the intra- and inter-atomic exchange interactions as well as correlated hopping, which allows us to describe the metallic paramagnetic-ferromagnetic transition with a realistic relationship between the above-mentioned exchange inter… Show more

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Cited by 9 publications
(5 citation statements)
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References 24 publications
(40 reference statements)
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“…Surprisingly similar behavior of magnetization as a function of d-band filling has been observed experimentally in the itinerant ferromagnetic systems 1xx2 FeCoS − and 1xx2CoNiS −[10]. Also similar behavior of magnetization has been seen in the theoretical work of Didukh et al[11] in their study of doubly orbitally degenerate generalized Hubbard model.…”
supporting
confidence: 77%
“…Surprisingly similar behavior of magnetization as a function of d-band filling has been observed experimentally in the itinerant ferromagnetic systems 1xx2 FeCoS − and 1xx2CoNiS −[10]. Also similar behavior of magnetization has been seen in the theoretical work of Didukh et al[11] in their study of doubly orbitally degenerate generalized Hubbard model.…”
supporting
confidence: 77%
“…At the same time, the majority of the results in the case of degenerated band (see for example [30][31][32][33][34][35]) are devoted only to a "standard" generalization of the degenerate Hubbard model. Besides, taking into account the correlated hopping essentially enriches the properties of the model (see [36][37][38]). …”
Section: Introductionmentioning
confidence: 99%
“…Together with evidence from the one orbital model we can conclude that these oscillations, appearing when doping the Néel state at half filling, are indeed signs of an incommensurate spin density wave 33,34,35 . For occupations of n 1.5 the physical situation starts to become influenced by the double exchange mechanism 36,37 and we thus expect to find ferromagnetic order 38,39,40,41,42,43,44,45 . Figure 1 and 2 FIG.…”
Section: A Filling Range 1 < N ≤mentioning
confidence: 95%