Please use this identifier to cite or link to this item: https://repositorio.ufrn.br/handle/123456789/28840
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dc.contributor.authorFerraz Filho, Álvaro-
dc.contributor.authorKochetov, Evgeny-
dc.date.accessioned2020-04-29T20:56:07Z-
dc.date.available2020-04-29T20:56:07Z-
dc.date.issued2013-01-02-
dc.identifier.citationFERRAZ FILHO, A.; KOCHETOV, E.A. . Comment on Z_{2}-slave-spin theory for strongly correlated fermions . Physical Review. B, Condensed Matter and Materials Physics, v. 87, p. 037101, 2013. Disponível em: https://journals.aps.org/prb/abstract/10.1103/PhysRevB.87.037101. Acesso em: 02 abr. 2020.pt_BR
dc.identifier.urihttps://repositorio.ufrn.br/jspui/handle/123456789/28840-
dc.languageenpt_BR
dc.publisherPHYSICAL REVIEW Bpt_BR
dc.subjectTeoria do spin Z2pt_BR
dc.titleComment on “Z2-slave-spin theory for strongly correlated fermions”pt_BR
dc.typearticlept_BR
dc.identifier.doi10.1103/PhysRevB.87.037101-
dc.description.resumoThe authors of Ref. 1 introduced a new slave-spin (SS) mean-field (MF) approach to the Hubbard model of strongly correlated electrons in terms of Ising spins and standard fermion operators by constructing an enlarged Hilbert space with both physical and unphysical states. The purpose of this construction is clear: this formulation involves a much smaller number of slave fields, compared with more standard slave particle frameworks. In this way, the complexity of the original model is reduced to a more readily tractable system of Ising spins in a transverse field coupled to free fermions. In this Comment, we show that the unphysical states are not properly excluded, and despite the claimed good agreement with previous results, the consistency of their MF theory is unjustifiedpt_BR
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