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      Stability of Nagaoka phase, spin effective action and delocalized free holes

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          Abstract

          The Hubbard model in the limit of infinite \(U\) is investigated within a projected slave fermion representation and following a previous work of the author and collaborators \cite{BFK}. The stability of the Nagaoka's phase with respect to a non vanishing concentration of holes (\(\delta_h\)) is analyzed by envisaging the existence of a spin effective action for itinerant magnetism of the Hubbard model. It is considered that,as the hole doping increases away from the half filled insulating limit, free holes are expected to be more delocalized. Depending on treatment for the hopping: a ferromagnetic or anti-ferromagnetic ordering might arise and the Nagaoka's phase might have some stability with respect to \(\delta_h \neq 0\).

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          Mean Field Theory of the Square Lattice Antiferromagnetic Heisenberg Model

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            Superconductivity in Strongly Correlated Electronic Systems and Confinement versus Deconfinement Phenomenon

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              Superconductor-insulator transition driven by local dephasing

              We consider a system where localized bound electron pairs form an array of "Andreev"-like scattering centers and are coupled to a fermionic subsystem of uncorrelated electrons. By means of a path-integral approach, which describes the bound electron pairs within a coherent pseudospin representation, we derive and analyze the effective action for the collective phase modes which arise from the coupling between the two subsystems once the fermionic degrees of freedom are integrated out. This effective action has features of a quantum phase model in the presence of a Berry phase term and exhibits a coupling to a field which describes at the same time the fluctuations of density of the bound pairs and those of the amplitude of the fermion pairs. Due to the competition between the local and the hopping induced non-local phase dynamics it is possible, by tuning the exchange coupling or the density of the bound pairs, to trigger a transition from a phase ordered superconducting to a phase disordered insulating state. We discuss the different mechanisms which control this occurrence and the eventual destruction of phase coherence both in the weak and strong coupling limit.
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                Author and article information

                Journal
                01 March 2009
                Article
                10.1016/j.physb.2009.07.087
                0903.0178
                dec9f038-bd3a-4239-9a3d-dd12d6c6eb47

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
                Custom metadata
                4 pages, work presented in SCES 2008, August 2008, Buzius, BR
                cond-mat.str-el cond-mat.supr-con

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